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(public plots, sorted by author)
Last update: Jun 16, 2017
INDEX SUBJECT |
TITLE links to plots |
AUTHOR status: link to info |
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Author: A | ||
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04-005 EXOTICS pentaquark |
Mass values and experimental FWHM widths observed in various experiments for the $\Theta^+$ state. The inner error bars represent the statistical uncertainties, and the outer error bars represent the quadratic sum of the statistical and systematic uncertainties. (Some uncertainties for the widths are not available from the other experiments.) The hatched area corresponds to the weighted average of all data \pm1 standard deviation Feb 7, 2004 *Colour (eps) *Colour (pdf) |
A. Airapetian
final |
04-004 EXOTICS pentaquark |
Spectra of invariant mass $M_{pK^-}$ (top) and M_{pK^+} (bottom). A clear peak is seen for the \Lambda(1520) in the M_{pK^-} invariant mass distribution. However, no peak structure is seen for the hypothetical \Theta^{++} in the M_{pK^+} invariant mass distribution near 1.53GeV Feb 7, 2004 *Colour (eps) *Colour (pdf) |
A. Airapetian
final |
04-003 EXOTICS pentaquark |
Distribution in invariant mass of the $p \pi^+\pi^-$ system. The experimental data are represented by the filled circles with statistical error bars, while the fitted smooth curves result in the indicated position and \sigma width of the peak of interest. In panel a), the PYTHIA-6 Monte Carlo simulation is represented by the gray shaded histogram, the mixed-event model normalised to the PYTHIA-6 simulation is represented by the fine-binned histogram, and the fitted curve is described in the text. In panel b), a fit to the data of a Gaussian plus a third-order polynomial is shown Feb 7, 2004 *Colour (eps) *Colour (pdf) |
A. Airapetian
final |
04-002 EXOTICS pentaquark |
Invariant mass distribution of two oppositely charged pions. A window corresponding to \pm 2 \sigma is shown by the vertical lines Feb 7, 2004 *Colour (eps) *Colour (pdf) |
A. Airapetian
final |
02-040 VECTOR-MESONS general, rho |
Overlay plot for 02-036 showing theoretical model calculation according to hep-ph/0008109 for Nitrogen, red line is without recoil corrections and blue line with recoil corrections taken into account. Calculation was performed at \nu=12GeV, while HERMES <\nu> is 13.8 GeV Feb 26, 2002 *Colour *Colour (eps) *Colour (pdf) |
A. Airapetian
prelim |
02-039 VECTOR-MESONS general, rho |
Overlay plot for 02-036 showing theoretical model calculation according to hep-ph/0008109 for Neon, red line is without recoil corrections and blue line with recoil corrections taken into account. Calculation was performed at average \nu per bin Feb 26, 2002 *Colour *Colour (eps) *Colour (pdf) |
A. Airapetian
prelim |
02-038 VECTOR-MESONS general, rho |
Overlay plot for 02-036 showing theoretical model calculation according to hep-ph/0008109 for ^{3}He, red line is without recoil corrections and blue line with recoil corrections taken into account. Calculation was performed at \nu=12GeV, while HERMES <\nu> is 13.8 GeV Feb 26, 2002 *Colour *Colour (eps) *Colour (pdf) |
A. Airapetian
prelim |
02-037 VECTOR-MESONS general, rho |
Q^{2} dependence of coherent to incoherent cross-section ratios for He3, Nitrogen, Neon and Krypton targets. For Kr: Inner error bar denotes statistical uncertainty, outer error bar includes the systematic uncertainty added in quadrature. For He3, Nitrogen, Neon the systematic error bands are plotted seperately Feb 26, 2002 *Colour *Colour (eps) *Colour (pdf) |
A. Airapetian
prelim |
02-036 VECTOR-MESONS general, rho |
Q^{2} dependence of coherent to incoherent cross-section ratios for He3, Nitrogen, Neon and Krypton targets. Inner error bar denotes statistical uncertainty, outer error bar includes the systematic uncertainty added in quadrature Feb 26, 2002 *Colour *Colour (eps) *Colour (pdf) |
A. Airapetian
prelim |
02-035 VECTOR-MESONS general, rho |
Coherent to incoherent cross-section ratios in dependence of target atomic number for exclusive diffractive rho electro-production, points are for Deuteron, He3, Nitrogen, Neon and Krypton targets Feb 26, 2002 *Colour *Colour (eps) *Colour (pdf) |
A. Airapetian
prelim |
02-034 VECTOR-MESONS general, rho |
Diffractive slope parameter in exclusive rho^{0} production vs target atomic number. HERMES points are in red and includes Hydrogen, Deuteron, He3, Nitrogen, Neon and Krypton targets. Point from E665 experiment are shown with blue squares and combined statistical and systematic uncertainties Feb 26, 2002 *Colour *Colour (eps) *Colour (pdf) |
A. Airapetian
prelim |
97-025 VECTOR-MESONS xsec |
Ratio of coherent to incoherent cross section for ^{3}He as a function of Q^{2} 1997 *Colour *Colour (eps) *Colour (pdf) |
A. Airapetian
prelim |
07-037 HADRON-ATTENUATION |
Alpha parameter obtained from a fit to the A-dependence of charged pi, K, and p production from four heavy targets, as a function of nu and z May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-036 HADRON-ATTENUATION |
Alpha and Beta parameters obtained from a fit to the A-dependence of charged-pion (combined) production from four heavy targets, as a function of L_{c} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-035 HADRON-ATTENUATION |
Alpha parameter obtained from a fit to the A-dependence of charged-pion (combined) production from four heavy targets, in nu slices and as a function of z May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-034 HADRON-ATTENUATION |
Multiplicity ratio R_{A}^{h} for charged pions (combined) produced from four heavy targets, in nu slices as a function of L_{c} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-033 HADRON-ATTENUATION |
Multiplicity ratio R_{A}^{h} for charged pions (combined) produced from four heavy targets, in p_{t}^{2} slices as a function of nu, z, and Q^{2} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-032 HADRON-ATTENUATION |
Multiplicity ratio R_{A}^{h} for charged pions (combined) produced from four heavy targets, in nu slices as a function of z, Q^{2}, and p_{t}^{2} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-031 HADRON-ATTENUATION |
Multiplicity ratio R_{A}^{h} for charged pions (combined) produced from four heavy targets, in z slices as a function of nu, Q^{2}, and p_{t}^{2} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-030 HADRON-ATTENUATION |
Multiplicity ratio R_{A}^{h} for pi^{0} produced from four heavy targets, as a function of nu, z, and Q^{2} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-029 HADRON-ATTENUATION |
Multiplicity ratio R_{A}^{h} for charged pi, K, and p produced from four heavy targets, as a function of p_{t}^{2} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-028 HADRON-ATTENUATION |
Multiplicity ratio R_{A}^{h} for negatively-charged hadrons produced from four heavy targets, as a function of nu, z, and Q^{2} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-027 HADRON-ATTENUATION |
Multiplicity ratio R_{A}^{h} for positively-charged hadrons produced from four heavy targets, as a function of nu, z, and Q^{2} May 29, 2007 *Colour (eps) *Colour (pdf) *Data |
N. Akopov
final |
07-026 HADRON-ATTENUATION |
Diagram of the kinematic variables used in the analysis of deep inelastic hadron production from heavy nuclear targets May 29, 2007 *BW (eps) *BW (pdf) |
N. Akopov
final |
03-083 HADRON-ATTENUATION |
Primakoff angle distribution for pi^{0} on Kr and D targets at 12 GeV Jul 2, 2003 *Colour *Colour (eps) *Colour (pdf) |
Z.Akopov and M.Amarian
prelim |
03-059 G1 gdh |
Generalized GDH integral for the neutron vs Q^{2}, showing three published data sets: (1) DIS part only(from ^{3}He target (2) DIS + resonance parts from proton - deuteron (3) JLab results for DIS + resonance from ^{3}He May 20, 2003 *Colour (eps) *Colour (pdf) |
N. Akopov
final |
03-058 G1 gdh |
Generalized GDH integral for the Proton - Neutron difference vs Q^{2} May 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
N. Akopov
final |
03-057 G1 gdh |
Generalized GDH integral for neutron and proton targets vs Q^{2}, after dividing out the leading-twist Q^{2} dependence May 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
N. Akopov
final |
03-056 G1 gdh |
Generalized GDH integral for all targets (neutron, deuteron, proton) vs Q^{2} for all kinematic regions May 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
N. Akopov
final |
03-055 G1 gdh |
Generalized GDH integral for the neutron (= deuteron - proton) vs Q^{2} for the DIS region May 20, 2003 *BW (eps) *BW (pdf) |
N. Akopov
final |
03-054 G1 gdh |
Generalized GDH integral for the neutron (= deuteron - proton) vs Q^{2} for all kinematic regions May 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
N. Akopov
final |
03-053 G1 gdh |
Generalized GDH integral for the proton target vs Q^{2} for all kinematic regions May 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
N. Akopov
final |
03-052 G1 gdh |
Cross section difference Delta sigma for the proton target vs photon energy and for different Q^{2} bins May 20, 2003 *BW (eps) *BW (pdf) *Data |
N. Akopov
final |
03-051 G1 gdh |
Generalized GDH integral for the deuteron target vs Q^{2} for all kinematic regions May 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
N. Akopov
final |
03-050 G1 gdh |
Cross section difference Delta sigma for the deuteron target vs photon energy and for different Q^{2} bins May 20, 2003 *BW (eps) *BW (pdf) *Data |
N. Akopov
final |
03-049 G1 gdh |
Data-MC comparison of inclusive yield vs W^{2} in the resonance region May 20, 2003 *BW (eps) *BW (pdf) |
N. Akopov
final |
00-038 G1 gdh, resonance |
a) I(GDH) as a function of Q^{2} for various upper limits of integration: W^{2} < 4.2GeV2 (triangles), W^{2} < 45GeV2 (squares), and the total integral I(GDH) (circles). The curve is the Soffer-Teryaev model for the total integral. b) I(GDH) Q^{2} /(16 pi2 alpha) as a function of Q^{2}. For both panels, the error bars show the statistical uncertainties, and the white and the hatched bands at the bottom represent the systematic uncertainties for the total integral with and without the A2 contribution Sep 6, 2000 *BW (eps) *BW (pdf) |
N. Akopov
final |
00-037 G1 gdh, resonance |
The GDH integral as a function of Q^{2} for the region 1.0GeV2 < W^{2} < 4.2GeV2. The error bars show the statistical uncertainties. The white and the hatched bands represent the systematic uncertainties with and without the A2 uncertainty contribution. The dashed and the solid curves are predictions based on a Q^{2}-evolution of nucleon-resonance amplitudes Sep 6, 2000 *BW (eps) *BW (pdf) |
N. Akopov
final |
00-036 G1 gdh, resonance |
Comparison of the event distribution for W^{2} > 1GeV2 (squares) with the Monte-Carlo simulation (histogram). An overall normalisation factor was applied to the simulation to match the data. Also shown are the smeared distributions from the elastic, resonance and the deep inelastic regions. The vertical lines indicate the resonance region considered in the analysis Sep 6, 2000 *BW (eps) *BW (pdf) |
N. Akopov
final |
01-073a DVCS proton |
Plot 01-073 but including new contribution BH(N-Delta) which is plotted with pink color. The ratio of R=BH(N-Delta)/BH(N-N) was found to be on the level of 10% based on computation following paper by Frankfurt et al. hep-ph/9808449 for the average values of x,Q^{2} and t and in the range of Mx<1.7 GeV May 15, 2002 *Colour (eps) *Colour (pdf) |
J. Ely/M. Amarian
final |
06-026 DIAGRAM |
a the HERMES logo for Christmas Jun 3, 2006 *Colour (eps) *Colour (pdf) |
A. Andrus
final |
16-173 UNPOL-PDF sea-flavour |
The scaled charge-difference multiplicities dN^{K}^{diff}/ dN^{DIS}. (^{5}Q + ^{2}S)/[4(uv + dv)] of charged kaons in semi-inclusive DIS from a deuterium target, as a function of x_{B}, evaluated using various LO PDF sets [MSTW08 (squares), CTEQ6 (upward triangles), NNPDF3.0 (downward triangles), and NNPDF2.3 (circles)], compared with the LO predictions based on solely DSS FFs (crosses) and DSS FFs combined with unfavored kaon FFs constrained using HERMES data at high x_{B} (stars). As in the Comment [3], all points were evaluated at the average Q^{2} of each individual x_{B} bin Jun 4, 2016 *Colour (eps) *Colour (pdf) *Data |
E.C. Aschenauer et al
final |
16-172 UNPOL-PDF sea-flavour |
The Q^{2} dependence of the DSS favored u and \bar{s} (scaled by a factor 1/7) as well as the unfavored \bar{u} to K^{+} fragmentation functions. Note that for the DSS FF set D^{K^{+}}_\bar{u} = D^{K^{+}}_\bar{d} . Chosen Q^{2} values correspond to the average Q^{2} of the x_{B} bins in Figs. 3(ab) and 5 Jun 4, 2016 *Colour (eps) *Colour (pdf) *Data |
E.C. Aschenauer et al
final |
16-171 UNPOL-PDF sea-flavour |
K^{\prime} "multiplicities". Equation (5) evaluated in the same way as the crosses to the left, but for a range of scaled DSS unfavored nonstrange kaon FFs [using scaling factors from 0 (bottom) to 4 (top) as in Fig. 2 (left) in the Comment]. As in the Comment [3], all points were evaluated at the average Q^{2} of each individual x_{B} bin Jun 4, 2016 *Colour (eps) *Colour (pdf) *Data |
E.C. Aschenauer et al
final |
16-170 UNPOL-PDF sea-flavour |
K^{\prime} "multiplicities" corrected to 4\pi of charged kaons in semi-inclusive DIS from a deuterium target, as a function of x_{B}, evaluated with Eq. (4) using MSTW08 (squares), CTEQ6 (upward triangles), NNPDF3.0 (downward triangles), and NNPDF2.3 (full circles) LO PDF sets. Also shown are the LO predictions [e.g., Eq. (5)] using DSS FFs (crosses) or using the high-x_{B} HERMES data to constrain the unfavored \bar{u} and \bar{d} to K^{+} FFs (stars). For both the crosses and stars, S\int{dzD_{S}^{K}} from Ref. [1] and Q from NNPDF3.0 were used. Note that uncertainties on PDFs or FFs-when available at all-were not propagated, but only total experimental uncertainties Jun 4, 2016 *Colour (eps) *Colour (pdf) *Data |
E.C. Aschenauer et al
final |
16-169 UNPOL-PDF sea-flavour |
Born space in (x_{B}, Q^{2}) corresponding to the multiplicities reported in Ref. [2]. Kinematic regions covered by two data points with similar average kinematics, as discussed in the Comment [3], are superimposed (highlighted slices in either x_{B} or Q^{2}). Note that the color coding is logarithmic, and that most of the events [O(70%)] in either of the two bins are in fact not shared Jun 4, 2016 *Colour (eps) *Colour (pdf) |
E.C. Aschenauer et al
final |
16-168 UNPOL-PDF sea-flavour |
Comparison of the shapes of multiplicities corrected to 4\pi of charged kaons and pions in semi-inclusive DIS from a deuterium target, as a function of Bjorken x_{B}. The kaon multiplicities are scaled to agree with those of pions in the range of xB where both distributions flatten. Data are plotted at the average x_{B} of each individual x_{B} bin Jun 4, 2016 *Colour (eps) *Colour (pdf) |
E.C. Aschenauer et al
final |
07-038 PR-PLOT |
Average beam polarisation per fill for 2004-2007 2007 *Colour *Colour (eps) *Colour (pdf) |
E.C. Aschenauer
final |
06-066 PR-PLOT |
Average beam polarisation per fill for 2003-2006 2006 *Colour (eps) *Colour (pdf) |
E.C. Aschenauer
final |
06-024 EXPERIMENT spectrometer |
Side view of HERMES spectrometer configuration 1996-1997 May 29, 2005 *Colour (eps) *Colour (pdf) *Colour (fig) |
E.C. Aschenauer
final |
06-023 EXPERIMENT spectrometer |
Side view of HERMES spectrometer configuration 1998-2000 May 29, 2005 *Colour (eps) *Colour (pdf) *Colour (fig) |
E.C. Aschenauer
final |
06-022 EXPERIMENT spectrometer |
Side view of HERMES spectrometer configuration 2001-2005 Jan 18, 2002 *Colour (eps) *Colour (pdf) *Colour (fig) |
U. ELschenbroich/E.C. Aschenauer
final |
06-021 EXPERIMENT spectrometer |
Side view of HERMES spectrometer configuration 2006-2007 May 29, 2005 *Colour (eps) *Colour (pdf) *Colour (fig) |
E.C. Aschenauer
final |
05-133 PR-PLOT |
average beam polarisation per fill for 2000, 2003-2005 Nov 13, 2005 *Colour (eps) *Colour (pdf) |
E. C. Aschenauer
final |
03-080 TRANSVERSE |
suporting plot: the smc SSA for a transverse polarised target; more info from A. Bravar DIS 1999 proceedings page 520 Jun 2, 2002 *Colour (eps) *Colour (pdf) |
E.C. Aschenauer
final |
03-079 TRANSVERSE |
suporting plot: the smc results on transversity for H and D-target; more info from A. Bravar DIS 1999 proceedings page 520 Jun 2, 2002 *Colour (eps) *Colour (pdf) |
E.C. Aschenauer
final |
02-079 PR-PLOT |
average beam polarisation per fill for 1996 - 2000 Sep 8, 2002 *Colour (eps) *Colour (pdf) |
E. C. Aschenauer
final |
02-078 PR-PLOT |
Photo of the Volkspark with HERA put on top of the photo Sep 8, 2002 *Colour (eps) *Colour (pdf) |
E. C. Aschenauer
final |
02-077a PR-PLOT |
HERA-setup 2001 - 2007 (!!!) Sep 8, 2002 *Colour (eps) *Colour (pdf) |
E. C. Aschenauer
final |
02-077b PR-PLOT |
HERA-setup 1995 - 2000 (!!!) Sep 8, 2002 *Colour (eps) *Colour (pdf) |
E. C. Aschenauer
final |
02-075 PR-PLOT |
HERA-performance in 2000: end-of-fill running Jun 19, 2002 *Colour *Colour (eps) *Colour (pdf) |
E. C. Aschenauer
final |
01-050 HIGH-PT hadron pairs |
A-parallel vs Pt for K^+/- pairs at high Pt (hydrogen and deuterium targets) May 6, 2001 *Colour *Colour (eps) *Colour (pdf) |
E. Aschenauer
prelim |
01-049 HIGH-PT hadron pairs |
A-parallel vs Pt for h^+/- and pi^+/- pairs at high Pt (hydrogen and deuterium targets) Apr 25, 2001 *Colour *Colour (eps) *Colour (pdf) |
E. Aschenauer
prelim |
01-048 HIGH-PT hadron pairs |
A-parallel vs Pt for h^+/- and pi^+/- pairs at high Pt (deuterium target) Apr 25, 2001 *Colour *Colour (eps) *Colour (pdf) |
E. Aschenauer
prelim |
01-047 HIGH-PT hadron pairs |
A-parallel vs Pt for h^+/- and pi^+/- pairs at high Pt (hydrogen target) Apr 25, 2001 *Colour *Colour (eps) *Colour (pdf) |
E. Aschenauer
prelim |
99-088 DIAGRAM |
Diagram of kinematic planes and azimuthal angle phi for pion production in semi-inclusive DIS Nov 15, 1999 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
H. Avakian
final |
99-078 AZIMUTHAL pi-proton |
Single spin asymmetry A_{UL} for pi^{+} and pi^{-} production, binned in azimuthal angle phi May 9, 2001 *Colour *BW *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
H. Avakian
final |
99-067 AZIMUTHAL pi-proton |
Azimuthal sin(phi) and sin(2phi) moments of A_{UL} vs x, for pi^{+} production Nov 15, 1999 *BW (eps) *BW (pdf) |
H. Avakian
final |
99-066p AZIMUTHAL pi-proton |
Azimuthal sin(phi) moment of A_{UL} vs p_{T}, for pi^{+} (red squares) and pi^{-} (blue circles) production Nov 15, 1999 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
H. Avakian
final |
99-066x AZIMUTHAL pi-proton |
Azimuthal sin(phi) moment of A_{UL} vs x, for pi^{+} (red squares) and pi^{-} (blue circles) production Jan 26, 2000 *Colour (eps) *Colour (pdf) |
H. Avakian
final |
08-015 DVCS |
Model-dependent constraint on u-quark total angular momentum J_{u} vs d-quark total angular momentum J_{d}. WARNING: this plot is NOT supposed to be shown anymore at conferences. The Dual model is known to have a theoretical theoretical calculation error which makes the interpretation invalid. The remaining models on the plot (VGG) don't describe all Hermes data. Mar 13, 2008 *Colour (eps) *Colour (pdf) |
E. Avetisyan
final |
08-014 DVCS |
same as 08-011 (top rows) with curves based on calculations using Regge-inspired form of the t-dependence in the dual-parameterisation GPD model. WARNING: this plot is NOT supposed to be shown anymore at conferences. The Dual model is known to have a theoretical theoretical calculation error which makes the interpretation invalid. Mar 13, 2008 *Colour (eps) *Colour (pdf) |
E. Avetisyan
final |
08-013 DVCS |
same as 08-010 (top row) with curves based on dual-parameterisation GPD model. WARNING: this plot is NOT supposed to be shown anymore at conferences. The Dual model is known to have a theoretical theoretical calculation error which makes the interpretation invalid. Mar 13, 2008 *Colour (eps) *Colour (pdf) |
E. Avetisyan
final |
08-012 DVCS |
Asymmetry amplitudes that are expected to be suppressed Mar 13, 2008 *Colour (eps) *Colour (pdf) |
E. Avetisyan
final |
08-011 DVCS |
Asymmetry amplitudes describing the dependence of the squared DVCS amplitudes and the interference term on the transverse target polarization, for the exclusive sample Mar 13, 2008 *Colour (eps) *Colour (pdf) *Data |
E. Avetisyan
final |
08-010 DVCS |
Asymmetry amplitudes describing the dependence of the interference term on the beam charge A_{C} for the exclusive sample Mar 13, 2008 *Colour (eps) *Colour (pdf) *Data |
E. Avetisyan
final |
08-009 DVCS |
Distributions in squared missing-mass from data with positron and electron beams and from Monte Carlo simulations Mar 13, 2008 *Colour (eps) *Colour (pdf) |
E. Avetisyan
final |
08-008 DVCS |
Momenta and azimuthal angles for exclusive electroproduction of photons in the target rest frame Mar 13, 2008 *BW (eps) *BW (pdf) |
E. Avetisyan
final |
08-007 DVCS |
Leading order diagrams for DVCS and Bethe-Heitler processes Mar 13, 2008 *BW (eps) *BW (pdf) |
E. Avetisyan
final |
07-016 AZIMUTHAL beam |
Definition of kinematic planes for semi-inclusive deep-inelastic scattering Apr 23, 2007 *BW (eps) *BW (pdf) |
E. Avetisyan
final |
Author: B | ||
Back to top | ||
05-112 DELTA-Q |
The inclusive asymmetry A_{1},d from the delta-q analysis and as published in the delta-q paper 2005 *Colour (eps) *Colour (pdf) INFO: supportive plot |
M. Beckmann (provided by L. De Nardo)
final |
05-068 DELTA-Q |
Korrelation matrix for the born level asymmetries on the deuteron Mar 28, 2005 *Data |
M. Beckmann
final |
05-067 DELTA-Q |
Korrelation matrix for the born level asymmetries on the proton Mar 28, 2005 *Data |
M. Beckmann
final |
05-060 DELTA-Q |
Matrices $n_{u}(i,j)=n_\spar(i,j)+n_\sant(i,j)$ for DIS events and SIDIS $\pi^+$ events on the proton. The binning shown corresponds to the 9 bins in $x$ that were used in the asymmetry and $\Delta q$ analysis Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-059 DELTA-Q |
The average strange quark helicity density $x\cdot[\Delta s(x)+\Delta\bar{s}(x)]/2$ from the isoscalar extraction method (full points). For comparison the open symbols denote the results from a five parameter fit (see text), which are offset horizontally for presentation. The band in the bottom part gives the total systematic uncertainty on the results from the isoscalar extraction. The dark shaded area corresponds to the uncertainty from the input asymmetries, and the open part relates to the uncertainty in $\lambda_{s}$ Mar 28, 2005 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
05-058 DELTA-Q |
The semi--inclusive Born level asymmetry $A_{1,d}^{K^+ + K^-}$ for the total charged kaon flux on a deuterium target, corrected for instrumental smearing and QED radiative effects. The uncertainties are presented analogously to Fig. 13 Mar 28, 2005 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
05-057 DELTA-Q |
The flavor asymmetry in the helicity densities of the light sea evaluated at $Q_{0}^{2}=2.5\,\GeV^{2}$. The data are compared with predictions in the $\chi$QSM and a meson cloud model \cite{Cao:2003}. The solid line with the surrounding shaded band show the $\chi$QSM prediction together with its $\pm 1\,\sigma$ uncertainties while the dash--dotted line shows the prediction in the meson cloud model. The uncertainties in the data are presented as in Fig. 19 Mar 28, 2005 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
05-056 DELTA-Q |
The quark helicity distributions $x\,\Delta q(x,Q_{0}^{2})$ evaluated at a common value of $Q^{2}_{0}=2.5\,\GeV^{2}$ as a function of $x$. The dashed line is the GRSV2000 parameterization (LO, valence scenario) scaled with $1/(1+R)$ and the dashed--dotted line is the Bl\"umlein--B\"ottcher (BB) parameterization (LO, scenario 1) Mar 28, 2005 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
05-055 DELTA-Q |
The quark polarizations in the 5 parameter $\times$ 9 $x$--bins fit. The polarizations, shown as a function of $x$, were computed from the HERMES inclusive and semi--inclusive asymmetries. The error bars are the statistical uncertainties. The band represents the total systematic uncertainty, where the light gray area is the systematic error due to the uncertainties on the fragmentation model, and the dark gray area is from the contribution of the Born asymmetries Mar 28, 2005 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
05-054 DELTA-Q |
Purities for positive and negative pions and kaons on a proton and a free neutron target. Each column corresponds to scattering off a certain quark flavor. The shaded bands indicate the estimated systematic uncertainties due to the fragmentation parameters. The estimate derives from a comparison of two parameter sets Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-053 DELTA-Q |
Multiplicities of charged pions and kaons in the HERMES acceptance compared with Monte Carlo data as function of $z$. Statistical uncertainties in the data are too small to be visible. The multiplicities shown were not corrected for radiative and instrumental effects Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-052 DELTA-Q |
Born level Monte Carlo asymmetries on the proton in the experimental acceptance and in $4\pi$. The left hand plot compares the semi--inclusive asymmetries $A_{1,p}^{\pi^+}$ and the right hand plot the semi--inclusive asymmetries $A_{1,p}^{\pi^-}$. The asymmetries in the experimental acceptance also include the hadron momentum cut. For display purposes the full data points have been offset horizontally. The lower panels present the same data in the form of the difference in the asymmetries divided by the total experimental uncertainty $\sigma_{born}$ in the corresponding measured Born asymmetry Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-051 DELTA-Q |
The semi--inclusive Born asymmetries for positive and negative pion production on the proton as a function of $z$. The error bars indicate the statistical uncertainties and the error band represents the systematic uncertainties. The solid line is the z dependence from the Monte Carlo simulation of the asymmetries Mar 28, 2005 *BW (eps) *BW (pdf) *Data |
M. Beckmann
final |
05-050 DELTA-Q |
The inclusive and semi--inclusive Born level asymmetries on the deuteron. One data point at $x = 0.45$ for the $K^-$ asymmetry including its large error bar is outside the displayed range; all data points are listed in XIII Mar 28, 2005 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
05-049 DELTA-Q |
The inclusive and semi--inclusive Born level asymmetries on the proton, corrected for instrumental smearing and QED radiative effects. The error bars give the statistical uncertainties, and the shaded bands indicate the systematic uncertainty. The open squares show the positive and negative hadron asymmetries measured by the SMC collaboration, limited to the HERMES $x$--range Mar 28, 2005 *Colour (eps) *BW (eps) *BW (pdf) *Data |
M. Beckmann
final |
05-048 DELTA-Q |
Uncertainty inflation caused by detector smearing and QED radiative effects. The left hand panel shows the uncertainty inflation of the inclusive asymmetry for the proton and the right hand panel that of the positive pion asymmetry. In both panels the open triangles present the uncertainty inflation caused by detector effects, the open squares present the inflation caused by QED radiative effects, and the filled circles show the total uncertainty inflation Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-047 DELTA-Q |
The observed asymmetries $A_\|$ and $A_\|^{\pi^+}$ on the proton target compared with the corresponding Born asymmetries. The Born asymmetries are offset horizontally for better presentation. See the text for details Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-046 DELTA-Q |
Cerenkov angles associated with the three particle hypotheses as a function of the particle momentum. The characteristic angles of \v{C}erenkov light emitted in the aerogel ($n=1.03$) are given by the solid lines. The characteristic angles for emission in the gas ($n=1.0014$) are shown as the dashed lines. The corresponding histogram entries are experimentally determined angles of a sample of SIDIS hadrons Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-045 DELTA-Q |
Identification efficiency and hadron contamination of the DIS lepton sample as a function of $x$. Because correlations between the responses of the PID detectors were neglected, the contaminations are uncertain by a factor of two. The deuteron data have slightly worse efficiencies and contaminations because of the better hadron--lepton discrimination of the threshold \v{C}erenkov counter compared to the RICH Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-044 DELTA-Q |
The distribution of the total $\mathrm{PID}$ value. This logarithmic ratio of probabilities includes the particle fluxes and the responses of all PID detectors. The left hand peak is the hadron peak, while the right hand peak originates from leptons. The limits that were applied in the analysis are shown as vertical lines Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-043 DELTA-Q |
Two--dimensional distribution of PID values for all particles in the acceptance. The quantities $\mathrm{PID3}$ and $\mathrm{PID5}$ are defined as $\mathrm{PID3}\equiv\mathrm{PID}_{cal}+\mathrm{PID}_{pre} +\mathrm{PID}_{ric}$ and $\mathrm{PID5}\equiv\mathrm{PID}_{trd} Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-042 DELTA-Q |
Tracking system resolution for lepton and hadron tracks for the detector configuration used since 1998. In the left panel the relative momentum resolution is displayed, and the right panel shows the resolution in the horizontal scattering angle $\theta_{x}$, both as a function of the track momentum $p$ Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-041 DELTA-Q |
Typical PID detector responses. The distributions are based on a small set of the data collected in 2000, except for the threshold \v{C}erenkov response, which was computed from a data set of similar size collected in 1997. The truncated mean is shown in the case of the TRD. The relative size of the lepton (dashed line) and hadron distributions (solid line) was scaled to the flux ratio in the respective data--taking periods to give a better idea of the level of contamination possible from each detector. The flux ratio of electrons to hadrons is typically $\sim 10\,\%$ for these data Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-040 DELTA-Q |
Side view of the HERMES spectrometer. The positron beam enters from the left. The spectrometer is split into two halves, one above the beam and one below, by a flux exclusion plate to protect the beams from the magnetic field. See the text for further details on the detectors Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-039 DELTA-Q |
Diagram of the HERMES polarized target. Shown are the atomic beam source (ABS), the target gas analyzer (TGA) and the Breit--Rabi polarimeter (BRP). SFT, MFT, and WFT label the strong, medium, and weak field transitions in the ABS and the BRP Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-038 DELTA-Q |
Schematic diagram of the HERA accelerator layout until 2000 with the location of the four experiments. Also shown are the locations of the spin--rotators and the two polarimeters Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
05-037 DELTA-Q |
Diagram of the deep-inelastic scattering process. The incoming lepton emits a virtual photon which is absorbed by one of the quarks in the nucleon. In the case depicted, the struck quark fragments into a pion in the final state. In semi--inclusive processes, the scattered lepton and part of the hadronic final state are detected in coincidence Mar 28, 2005 *BW (eps) *BW (pdf) |
M. Beckmann
final |
03-115 DELTA-Q |
The light quark sea flavor asymmetry x*(\Delta \bar{u} - \Delta\bar{d}) in the helicity distributions, at Q^{2}=2.5 GeV^{2} compared to a theoretical prediction from the chiral quark soliton model (dashed curve with theoretical uncertainty band). The experimental error bars and bands have the same meaning as in Fig.2 (03-114) Nov 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
03-114 DELTA-Q |
Quark helicity distributions at Q^{2}=2.5 GeV^{2}, as a function of Bjorken x, compared to two LO QCD fits to previously published inclusive data shown as dashed GRSV-2000 (standard scenario) and dot-dashed BB (scenario~1) curves. The error bars are statistical and the bands at the bottom represent the systematic uncertainties, where the light area is the contribution due to the uncertainties of the fragmentation model, and the dark area is the contribution due to those of the asymmetries Nov 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
03-113 DELTA-Q |
Virtual photo-absorption asymmetries A^{h}_{1} for semi-inclusive DIS on the deuterium target as a function of Bjorken x, for identified charged pions (compared to all charged hadrons from SMC in the x-range of the present experiment), and for identified charged kaons. The error bars are statistical, and the bands at the bottom represent the systematic uncertainties. Two data points for K^- at large x are off-scale with large error bars Nov 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
M. Beckmann
final |
03-081 DELTA-Q |
scheme showing how the purities are extracted from Monte Carlo Jun 8, 2002 *Colour (eps) *Colour (pdf) |
M. Beckmann
final |
02-074 DELTA-Q |
Expected stat. precision on x*Delta-q for the 5 flavour decomposition when using all 1996-2000 data and ^{2}M DIS events in addition on a long. pol. hydrogen target with RICH hadron identification May 15, 2002 *Colour *Colour (eps) *Colour (pdf) |
J. Wendland/M. Beckmann
final |
02-074a DELTA-Q |
Expected stat. precision on x*Delta-q for the 5 flavour decomposition when using all 1996-2000 data and ^{4}M DIS events in addition on a long. pol. hydrogen target with RICH hadron identification May 15, 2002 *Colour *Colour (eps) *Colour (pdf) |
J. Wendland/M. Beckmann
final |
02-074b DELTA-Q |
Expected stat. precision on (Delta u_{bar})-(Delta d_{bar}) when using all 1996-2000 data plus ^{2}M / ^{4}M extra DIS events with RICH info. Both scenarios are shown in this plot May 15, 2002 *Colour *Colour (eps) *Colour (pdf) |
J. Wendland/M. Beckmann
final |
99-044 DIAGRAM |
Diagram of polarized semi-inclusive DIS 1999 *Colour (eps) *Colour (pdf) *Colour (fig) |
M. Beckmann
final |
97-028 EXPERIMENT polarimeters |
risetime curve transverse polarimeter 1997 *Colour *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
M. Beckmann
final |
11-026 LAMBDA-POL longitudinal |
Results on integrated D_{Lx} and D_{Lz} in the coordinate system with z axis along the vritual photon momentum Apr 27, 2011 *Colour (eps) *Colour (pdf) |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-025 LAMBDA-POL longitudinal |
Results on integrated D_{Lx} and D_{Lz} in the coordinate system with z axis along the anti-lambda momentum Apr 27, 2011 *Colour (eps) *Colour (pdf) |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-024 LAMBDA-POL longitudinal |
The x_{B} -dependence of the longitudinal component of D_{LL}' in the two coordinate systems (w.r.t. virtual photon or anti-lambda momentum) Apr 27, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-023 LAMBDA-POL longitudinal |
The x_{B}-dependence of the transverse component of D_{LL}' in the two coordinate systems (w.r.t. virtual photon or anti-lambda momentum) Apr 27, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-022 LAMBDA-POL longitudinal |
The x_{F}-dependence of the longitudinal component of D_{LL}' in the two coordinate systems (w.r.t. virtual photon or anti-lambda momentum) Apr 27, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-021 LAMBDA-POL longitudinal |
The x_{F}-dependence of the transverse component of D_{LL}' in the two coordinate systems (w.r.t. virtual photon or anti-lambda momentum) Apr 27, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-020 LAMBDA-POL longitudinal |
The z-dependence of the longitudinal component of D_{LL}' in the two coordinate systems (w.r.t. virtual photon or anti-lambda momentum) Apr 27, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-019 LAMBDA-POL longitudinal |
The z-dependence of the transverse component of D_{LL}' in the two coordinate systems (w.r.t. virtual photon or anti-lambda momentum) Apr 27, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-018 LAMBDA-POL longitudinal |
The y-dependence of the longitudinal component of D_{LL}' in the two coordinate systems (w.r.t. virtual photon or anti-lambda momentum) Apr 27, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-017 LAMBDA-POL longitudinal |
The y-dependence of the transverse component of D_{LL}' in the two coordinate systems (w.r.t. virtual photon or anti-lambda momentum) Apr 27, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-016 LAMBDA-POL longitudinal |
The longitudinal component of D_{LL}' compared to world data Apr 27, 2011 *Colour (eps) *Colour (pdf) |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
11-015 LAMBDA-POL longitudinal |
The transverse component of D_{LL}' compared to world data Apr 27, 2011 *Colour (eps) *Colour (pdf) |
S. Belostotski, Yu. Naryshkin and D. Veretennikov
prelim |
96-051 LAMBDA fragmentation |
Lambda mass peak 1996 *Colour *Colour (eps) *Colour (pdf) |
S.Belostotski
prelim |
99-107 DIAGRAM |
Diagram of diffractive rho production, showing rho decay to pi^{+} pi^{-} Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-106 VECTOR-MESONS spin transfer, rho |
Invariant mass spectrum for diffractive rho production from ^{3}He Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-105 VECTOR-MESONS spin transfer, rho |
DeltaE spectrum for diffractive rho production from ^{3}He Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-103 VECTOR-MESONS spin transfer, rho |
Parametrization of DeltaE spectrum for double-diffractive dissociation (arbitrary units) Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-102 DIAGRAM |
Diagram of the angles theta, phi, and Phi used to describe diffractive rho production and decay Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-101 VECTOR-MESONS spin transfer, rho |
Phase difference delta between the longitudinal and transverse amplitudes for diffractive rho production from ^{3}He Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-100 VECTOR-MESONS spin transfer, rho |
Acceptance corrected cos(theta) spectrum for diffractive rho production from ^{3}He Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-099 VECTOR-MESONS spin transfer, rho |
Acceptance corrected psi spectrum for diffractive rho production from ^{3}He Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-098n VECTOR-MESONS spin transfer, rho |
Spin density matrix elements r^{04}_{00} and r^{1}_{1-1} for diffractive rho production from ^{3}He Nov 7, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-097 VECTOR-MESONS spin transfer, rho |
Acceptance corrected phi spectrum for diffractive rho production from ^{3}He Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-096n VECTOR-MESONS spin transfer, rho |
Spin density matrix elements r^{04}_{1-1} and r^{3}_{1-1} for diffractive rho production from ^{3}He Nov 7, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-095 VECTOR-MESONS spin transfer, rho |
Acceptance corrected Phi spectrum for diffractive rho production from ^{3}He Mar 16, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-094n VECTOR-MESONS spin transfer, rho |
Spin density matrix elements Tr(r^{1}), Tr(r^{5}), and Tr(r^{8}) for diffractive rho production from ^{3}He Nov 7, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
99-093n VECTOR-MESONS spin transfer, rho |
Ratio R = sigma_{L}/sigma_{T} for diffractive rho production from ^{3}He Nov 7, 2000 *BW (eps) *BW (pdf) |
E. Belz
final |
06-051 G1 |
World data for the structure function g_{1} of the deuteron as function of Q^{2} (Q^{2} >1 GeV^{2}) for fixed x 2006 *Colour *Colour (eps) *Colour (pdf) |
H. Boettcher
final |
06-050 G1 |
World data for the structure function g_{1} of the proton as function of Q^{2} (Q^{2} >1 GeV^{2}) for fixed x 2006 *Colour *Colour (eps) *Colour (pdf) |
H. Boettcher
final |
09-036a VECTOR-MESONS spin density matrix elements |
Q^{2} dependence of the longitudinal-to-transverse cross section ratio for exclusive rho^{0} production on the proton. R^{04} calculated from the SDME r^{04}_{00} according to Eq.69. HERMES proton data (filled squares) are compared to measurements of CLAS, Cornell, E665, H1, and ZEUS. The more recent CLAS data (small squares) are from a narrow bin in x_{B} with approximately the same < x_{B} > as the HERMES data, which are integrated over the x_{B} acceptance. (See publication for references) Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-036b VECTOR-MESONS spin density matrix elements |
Q^{2} dependence of the longitudinal-to-transverse cross section ratio for exclusive rho^{0} production on the proton. $R^{04}$ for ZEUS (triangles) and R^{NPE} for HERMES (squares), fitted separately according to Eq.76. For all data points, total uncertainties are shown. Theoretical calculations of R_{0} = |T_{00}|^2/|T_{11}|^2 are shown as dashed line at W=5GeV; the uncertainties arising from the uncertainties in the parton distribution functions are shown as a shaded band. (See publication for references) Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-035a VECTOR-MESONS spin density matrix elements |
Q^{2} dependence of the longitudinal-to-transverse cross section ratio measured at HERMES. Proton results. Filled symbols represent the value of R^{04} calculated from r^{04}_{00} (Eq.69), open symbols correspond to the true value of R calculated according to Eqs.70,72, and crosses (diamonds) represent R^{NPE} Eq.75. Total uncertainties are shown, calculated by combining the statistical and systematic uncertainties in quadrature. The data points for R and R^{NPE} are presented with a small horizontal offset to improve their visibility Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-035b VECTOR-MESONS spin density matrix elements |
As entry 09-035a, but deuteron results Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-034 VECTOR-MESONS spin density matrix elements |
Ratios of certain helicity-flip amplitudes to the square root of the sum of all amplitudes squared: \tau_{01}, \tau_{10}, and \tau_{1-1}. HERMES results on proton (filled squares) and deuteron (filled circles) are calculated according to Eqs.59-61, while results from DESY, SLAC'79, SLAC'74, ZEUS BPS, ZEUS DIS and H1 are calculated according to Eqs.70,72. (See publication for references) For HERMES (other experiments) systematic uncertainties are combined in quadrature with (without) accounting for correlations between the SDMEs. The HERMES deuteron and SLAC'74 data points are presented with a small horizontal offset to improve their visibility Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-033 VECTOR-MESONS spin density matrix elements |
Average values of u_{1}, u_{2} and u_{3} calculated according to Eqs.52-54 from HERMES proton (filled squares) and deuteron (filled circles). SDMEs are shown together with the values calculated from published SDMEs from DESY, SLAC'79, SLAC'74, ZEUS BPS, ZEUS DIS, and H1. (See publication for references) For HERMES (other experiments) systematic uncertainties are combined in quadrature with (without) accounting for correlations between the SDMEs. The HERMES deuteron and SLAC'74 data points are presented with a small horizontal offset to improve their visibility Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-032a VECTOR-MESONS spin density matrix elements |
The Q^{2} dependence of u_{1} = 1-r_{00}^{04} + 2 r_{1-1}^{04} - 2 r_{11}^{1} - 2 r_{1-1}^{1} for proton (filled squares) and deuteron (filled circles) data. The values of u_{1} for yields integrated over the range 1GeV^{2} < Q^{2} < 7GeV^{2} are shown as open symbols. The inner (outer) error bars represent the statistical (total) uncertainties Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-032b VECTOR-MESONS spin density matrix elements |
As entry 09-032a, but t' dependence Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-031 VECTOR-MESONS spin density matrix elements |
Q^{2} and t' dependences of the "Class E" SDMEs describing the interference of the double-helicity-flip transition gamma^*_{-T} -> rho^{0}_{T} and the dominant transition gamma^*_T -> rho^{0}_{T}. Filled squares (circles) correspond to proton (deuteron) data. Total uncertainties are depicted, calculated as statistical and systematic uncertainties combined in quadrature Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-030 VECTOR-MESONS spin density matrix elements |
Q^{2} and t' dependences of the "Class D" SDMEs describing the interference of the helicity-flip transition gamma^*_L -> rho^{0}_{T} and the dominant transition gamma^*_T -> rho^{0}_{T}. Filled squares (circles) correspond to proton (deuteron) data. Total uncertainties are depicted, calculated as statistical and systematic uncertainties combined in quadrature Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-029 VECTOR-MESONS spin density matrix elements |
Q^{2} and t' dependence of the "Class C" SDMEs describing the interference of the helicity-flip transition gamma^*_T -> rho^{0}_{L} and one of the dominant helicity-conserving transition. Filled squares (circles) correspond to proton (deuteron) data. Total uncertainties are depicted, calculated as statistical and systematic uncertainties combined in quadrature Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-028 VECTOR-MESONS spin density matrix elements |
The Q^{2} dependence of the phase difference \delta between T_{11} and T_{00} amplitudes calculated according to Eq.50 for the proton (filled squares) and deuteron (filled circles) data. The values of \delta, for yields integrated over the range 1GeV^{2} < Q^{2} < 7 GeV^{2}, are shown as open symbols. The inner (outer) bars represent the statistical (total) uncertainty Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-027 VECTOR-MESONS spin density matrix elements |
Q^{2} and t' dependences of the "Class B" SDMEs describing the interference of the dominant transitions gamma^*_L -> rho^{0}_{L} and gamma^*_T -> rho^{0}_{T}. Filled squares (circles) correspond to proton (deuteron) data. Total uncertainties are depicted, calculated as statistical and systematic uncertainties combined in quadrature Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-026 VECTOR-MESONS spin density matrix elements |
Q^{2} and t' dependences of the "Class A" SDMEs describing the dominant transitions gamma^*_L -> rho^{0}_{L} and gamma^*_T -> rho^{0}_{T}. Filled squares (circles) correspond to proton (deuteron) data. Total uncertainties are depicted, calculated as statistical and systematic uncertainties combined in quadrature. Deuterium data points are presented with a small horizontal offset to improve their visibility Jun 29, 2009 *BW (eps) *BW (pdf) INFO: The data values are contained in the file attached to entry 09-025. |
A. Borissov
final |
09-025 VECTOR-MESONS spin density matrix elements |
The 23 SDMEs extracted from rho^{0} data: proton (squares) and deuteron (circles) in the entire HERMES kinematics with < x_{B}>=0.08, < Q^{2}>= 1.95GeV^{2}, <-t'>=0.13GeV^{2}. The SDMEs are multiplied by prefactors in order to represent the normalized leading contribution of the corresponding amplitude. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature. SDMEs measured with unpolarized (polarized) beam are displayed in the unshaded (shaded) areas. The vertical dashed line at zero is indicated for SDMEs expected to be zero under the hypothesis of SCHC Jun 29, 2009 *BW (eps) *BW (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
A. Borissov
final |
09-024 VECTOR-MESONS spin density matrix elements |
Shape comparison of the distributions in W, Q^{2}, t' and P_{\pi^+}, the momentum of the pi^+ from rho^{0} decay in the laboratory system, for the hydrogen data sample (squares). The shaded areas show rhoMC results using the extracted 23 SDMEs as input for the simulation, normalized to the data. Background has been subtracted from the data Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
09-023a VECTOR-MESONS spin density matrix elements |
Angular distributions with common arbitrary normalization for rho^{0} meson production and decay. Data points represent the positive helicity sample of the proton data. The dotted lines represent isotropic input Monte Carlo distributions as modified by the HERMES acceptance, while the dashed lines are the results of the 23-parameter fit. Here 16 bins are chosen for a more detailed comparison. The data correspond to the full kinematic region of the analysis Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
09-023b VECTOR-MESONS spin density matrix elements |
As entry 09-023a, but for deuteron data Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
09-022 VECTOR-MESONS spin density matrix elements |
Distribution of \Delta E for the 1996-2005 hydrogen data sample shown for four intervals in t' after application of all event selection requirements, except the one for \Delta E. The shaded areas represent the SIDIS background calculated by PYTHIA, normalized to the data in the region 2GeV < \Delta E < 20GeV Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
09-021 VECTOR-MESONS spin density matrix elements |
The distribution of rho^{0} mesons in \Delta E, and t' from the 1996-2005 hydrogen data sample in the range 1GeV^{2} < Q^{2} < 7GeV^{2} Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
09-020 VECTOR-MESONS spin density matrix elements |
Two-pion invariant mass distribution in the spectrometer acceptance, fitted with a skewed Breit-Wigner function (solid line). The dotted line represents a constant background contribution Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
09-019 VECTOR-MESONS spin density matrix elements |
Definition of angles in the process gamma^* N -> rho^{0} N' -> pi^+ pi^- N'. Here \Phi is the angle between the rho^{0} production plane and the lepton scattering plane in the "hadronic" center-of-mass system of virtual photon and target nucleon. \Theta and \phi are polar and azimuthal angles of the decay \pi^+ in the vector meson rest frame Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
09-018 VECTOR-MESONS spin density matrix elements |
Examples of a) a two-gluon exchange diagram and b) a quark-exchange diagram, shown for the lowest order in the strong coupling constant alpha_{s} Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
09-017 VECTOR-MESONS spin density matrix elements |
Feynman diagram of a generic t-channel exchange process for gamma^* N -> rho^{0} N' Jun 29, 2009 *BW (eps) *BW (pdf) |
A. Borissov
final |
03-063 VECTOR-MESONS xsec |
Same as Fig. 3 (03-062) but now for incoherent production on ^{14}N May 20, 2003 *Colour (eps) *Colour (pdf) |
S. Borissov
final |
03-062 VECTOR-MESONS xsec |
Nuclear transparency as a function of Q^{2} in coherence length bins for coherent rho^{0} production on ^{14}N May 20, 2003 *Colour (eps) *Colour (pdf) |
S. Borissov
final |
03-061 VECTOR-MESONS xsec |
Scatter plot of Q^{2} versus coherence length for exclusive rho^{0} production on ^{14}N and H May 20, 2003 *Colour (eps) *Colour (pdf) |
S. Borissov
final |
03-060 VECTOR-MESONS xsec |
Nuclear transperency as a function of coherence length for coherent and incoherent rho^{0} production on ^{14}N May 20, 2003 *Colour (eps) *Colour (pdf) *Data |
S. Borissov
final |
00-054 VECTOR-MESONS xsec, phi |
Total cross section for phi production vs W, overlaid with world data at various W and Q^{2} values Sep 10, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Borissov
prelim |
00-053 VECTOR-MESONS xsec, phi |
Total cross section for phi production vs Q^{2}, overlaid with data from ZEUS at W = 90 GeV. Each data set is overlaid with a fit based on the VDM, to the form (1 + Q^{2}/M^{2})^-m Sep 10, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Borissov
prelim |
00-050 VECTOR-MESONS xsec, phi |
Total, longitudinal, and transverse phi production cross-sections vs Q^{2}, overlaid with fits to the form (1 + Q^{2}/M^{2})^-m Sep 10, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Borissov
prelim |
00-049 VECTOR-MESONS xsec, rho |
Total, longitudinal, and transverse rho production cross-sections vs Q^{2}, overlaid with fits to the form (1 + Q^{2}/M^{2})^-m Sep 10, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Borissov
prelim |
00-048 VECTOR-MESONS xsec |
Total cross section for rho and phi production vs (Q^{2}+M^{2})/4, compared with data from H1 and ZEUS at W=75 GeV. The HERMES data at W = 5 have been 'corrected' to W = 75 using the soft-Pomeron dependence W^{delta}, with delta = 0.22 Sep 10, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Borissov
prelim |
00-047 VECTOR-MESONS xsec, phi |
Ratio of phi/rho total cross-section vs Q^{2}, compared with world data at various W values Sep 10, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Borissov
prelim |
00-044 VECTOR-MESONS xsec, rho |
The longitudinal component of the virtual-photoproduction cross section for rho^{0} production versus W at average Q^{2} values of 2.3 (left) and 4.0 GeV^{2} (right) Sep 7, 2000 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
A. Borissov
final |
00-043 VECTOR-MESONS xsec, rho |
The virtual-photoproduction cross section for rho^{0} production versus W at average Q^{2} values of 0.83, 1.3, 2.3 and 4.0 GeV^{2} (from top to bottom) Sep 7, 2000 *Colour (eps) *Colour (pdf) |
A. Borissov
final |
00-042 VECTOR-MESONS xsec, rho |
The virtual-photoproduction cross section for rho^{0} production on H versus Q^{2} Sep 7, 2000 *BW (eps) *BW (pdf) |
A. Borissov
final |
00-041 VECTOR-MESONS xsec, rho |
The virtual-photoproduction cross section for exclusive rho^{0} production versus W for the indicated values of average Q^{2} Sep 7, 2000 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
A. Borissov
final |
00-040 VECTOR-MESONS xsec, rho |
Invariant mass spectrum of the two oppositely charged hadrons assuming that they are pions Sep 7, 2000 *BW (eps) *BW (pdf) |
A. Borissov
final |
00-039 VECTOR-MESONS xsec, rho |
Missing energy spectra for leptoproduction of rho^{0} mesons off H at an incident energy of 27.5 GeV Sep 7, 2000 *BW (eps) *BW (pdf) |
A. Borissov
final |
99-104 VECTOR-MESONS spin transfer, rho |
t' spectrum for diffractive rho production from ^{3}He Mar 16, 2000 *BW (eps) *BW (pdf) |
A. Borissov
final |
99-018 VECTOR-MESONS xsec, rho |
Photoproduction (Q^{2}=0) cross section vs W 1999 *Colour (eps) *Colour (pdf) |
A. Borissov
prelim |
99-079 EXPERIMENT charm upgrade |
Schematic diagram of the charm upgrade detectors Dec 13, 1999 *Colour *Colour (eps) *Colour (pdf) |
M. Bouwhuis
final |
99-049c DIAGRAM |
Feynman diagram of photon gluon fusion, producing charm quarks Feb 3, 2000 *Colour (eps) *Colour (pdf) *Colour (fig) |
M. Bouwhuis
final |
99-043u EXPERIMENT spectrometer |
Side view of HERMES spectrometer, including upgrade detectors Feb 3, 2000 *Colour *Colour (eps) *Colour (pdf) *Colour (fig) |
M. Bouwhuis
final |
12-042 DVCS proton |
Amplitudes of single-charge beam-helicity asymmetry extracted from pure sample obtained with recoil-proton reconstruction. The amplitudes are presented in projections of -t, xB, and Q^{2}. The overall results shown in the very left panel are extracted in a single kinematic bin covering the entire kinematic acceptance. Statistical (systematic) uncertainties are represented by error bars (bands). A separate scale uncertainty arising from the measurement of the beam polarization amounts to 1.96%. The theoretical models are evaluated at the average values of the kinematics. The thickness of the VGG lines represents the range bval = 1...infinity Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-041 DVCS proton |
Amplitudes of single-charge beam-helicity asymmetry in DVCS shown in projections of -t, xB, and Q^{2}. Statistical uncertainties are shown by error bars. The bands represent the systematic uncertainties of the amplitudes extracted from the pure sample. A separate scale uncertainty arising from the measurement of the beam polarization amounts to 1.96%. Shown are amplitudes extracted from a) the pure sample (red circles, shown at their kinematic values), i.e., obtained with recoil-proton reconstruction; b) the unresolved-reference sample (blue triangles, shifted to the right for better visibility), i.e., without recoil-proton reconstruction but requiring its four-momentum to be in the recoil-detector acceptance; c) the unresolved sample (black stars, shifted to the left for better visibility), i.e., without requirements from recoil-detector acceptance and reconstruction. The latter two sets of amplitudes are subject to an average contribution of 14% and 12%, respectively, for associated processes Oct 19, 2012 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. The actually reconstructed kinematic values for every bin are also presented. |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-040 DVCS proton |
The fractional contributions from the BH process (closed symbols) and associated BH process (open symbols), for each of the exclusive samples. The fractional contributions are extracted from Monte Carlo simulations and are presented in the same kinematic binning as the asymmetry amplitudes. Symbols for the unresolved (unresolved-reference) sample are shifted to the left (right) for better visibility. If the points were plotted without such shifts, a difference would only be visible in the first -t bin Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-039 DVCS proton |
Left: unresolved; middle: unresolved-reference; right: pure sample. Experimental data, shown as data points (uncertainties covered by symbols), are compared to simulated data. In every panel, the contribution from BH events is indicated as dashed histogram, and the contributions from associated production and semi-inclusive background are shown as hatched histograms. The sum of the simulated distributions is shown as solid histogram Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-038 DVCS proton |
Distribution of the squared missing mass from experimental data for unresolved, unresolved-reference and pure exclusive event samples. The requirements applied on the squared missing mass in order to select (only) the unresolved and the unresolved-reference samples are indicated as vertical dashed-dotted lines. The exclusive signal is expected around the square of the proton mass, indicated as vertical dashed line Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-037 DVCS proton |
The polar-angle resolution versus momentum Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-036 DVCS proton |
The azimuthal-angle resolution versus momentum Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-035 DVCS proton |
The momentum resolution versus momentum for proton reconstruction by using only the information on the curvature in the magnetic field (circles) and by combining the information on curvature with energy deposition in the SSD (squares) Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-034 DVCS proton |
Schematic diagram of the Hermes recoil detector (cross-section view). The Hera lepton beamis perpendicular to the paper plane. The cross section of the target cell is shown as ellipse. The tracking layers are indicated, from inside to outside: inner and outer layers (in diamond shape) of the Silicon Strip Detector (SSD), inner and outer barrels (circles) of the Scintillating Fiber Tracker (SFT). Space-points are indicated by crosses. The SSD modules are located inside the vacuum chamber (dashed circle). The Photon Detector (PD) shown as a dash-dotted circle is not used in the present analysis. The magnet (not shown) surrounds the detector assembly. Also shown are examples of tracks reconstructed from two, three, and four space-points Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-033 DVCS proton |
Leading-order diagram for the channel ep -> ep\gamma for Bethe-Heitler (BH) processe Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-032 DVCS proton |
Leading-order diagram for the channel ep -> ep\gamma for deeply virtual Compton scattering (DVCS) process Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-031 DVCS proton |
Momenta and azimuthal angle for exclusive electroproduction of real photons in the target rest frame Oct 19, 2012 *Colour (eps) *Colour (pdf) |
J. Bowles, J. Burns, M. Murray, W.-D. Nowak, C. Riedl and S. Yaschenko
final |
12-019 DVCS |
Beam-helicity asymmetry in associated electroproduction of real photons ep->e gamma Delta+->e gamma n pi^{+} Jun 20, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 12-018 |
I. Brodski, E. Etzelmueller, A. Movsisyan and S. Yaschenko for recoil and DVCS groups
prelim |
12-018 DVCS |
Beam-helicity asymmetry in associated electroproduction of real photons ep->e gamma Delta+->e gamma p pi^{0} Jun 20, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry |
I. Brodski, E. Etzelmueller, A. Movsisyan and S. Yaschenko for recoil and DVCS groups
prelim |
98-068 CHARM d* |
Signal for D* --> D0 pi (96+97 data) 1998 *Colour *Colour (eps) *Colour (pdf) |
S. Brons
prelim |
03-123 F2 f2ratio |
The isoscalar-corrected ratio $R_{A} / R_{D}$ for several nuclei (A) with respect to deuterium as a function of $Q^{2}$. The HERMES and NMC data have been combined in the determination of $R_{A} / R_{D}$. The other data are the same as in Fig. 6 Aug 20, 2004 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-122 F2 f2ratio |
The isoscalar-corrected ratio $R_{A} / R_{D}$ for several nuclei (A) with respect to deuterium as a function of $Q^{2}$ for four different x bins. The open triangles ($^{12}$C) and crosses ($^{4}$He) have been derived from the NMC data using Eq.~3. The other SLAC and NMC data displayed have been derived from published values of $\Delta R = R_{A} - R_{D}$ and a parameterisation for $R_{D}$. The inner error bars represent the statistical uncertainty and include the correlated error in $F_{2}^{A}/F_{2}^{D}$. The outer error bars represent the quadratic sum of the statistical and systematic uncertainties. In the upper panel the HERMES results at the lowest $Q^{2}$ value have been suppressed because of its large error bar Aug 20, 2004 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-121 F2 f2ratio |
Ratio of isoscalar Born cross sections of inclusive deep-inelastic lepton scattering from nitrogen and deuterium (renormalised by 1.5%) as function of $\epsilon$ for fixed values of $x$. The error bars represent the statistical uncertainties Aug 20, 2004 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-120 F2 f2ratio |
Ratio of isoscalar Born cross sections of inclusive deep-inelastic lepton scattering from nucleus $A$ and $D$ as function of $Q^{2}$ for fixed values of $x$. The error bars represent the statistical uncertainties. The HERMES $^{14}$N/D data have been renormalised by 1.5% Aug 20, 2004 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-119 F2 f2ratio |
Ratio of isoscalar Born cross sections of inclusive deep-inelastic lepton scattering from nucleus $A$ and $D$ as function of $Q^{2}$ for fixed values of $x$. The error bars represent the statistical uncertainties. The HERMES $^{14}$N/D data have been renormalised by 1.5% Aug 20, 2004 *BW (eps) *BW (pdf) *Data |
A. Bruell
final |
03-118 F2 f2ratio |
Ratio of isoscalar Born cross sections of inclusive deep-inelastic lepton scattering from nucleus A and D versus x. The error bars represent the statistical uncertainties, the systematic uncertainties are given by the error bandsi (ordered as HERMES, SLAC, NMC). The HERMES $^3$He/D and $^{14}$N/D data have been renormalised by 1.5% Aug 20, 2004 *BW (eps) *BW (pdf) *Data |
A. Bruell
final |
03-117 F2 f2ratio |
Comparison between data (points) and MC simulation (histogram) for the fractional change in the cross section ratios when treating the upper and lower HERMES detector halves independently Aug 20, 2004 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-116 F2 f2ratio |
Ratio of track reconstruction efficiencies in $^1$H, $^3$He, $^{14}$N and $^{84}$Kr with respect to $^2$H as function of x Aug 20, 2004 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-091 F2 f2ratio |
The isoscalar-corrected ratio R_{A} / R_{D} for several nuclei (A) with respect to deuterium as a function of Q^{2} Aug 11, 2003 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-090 F2 f2ratio |
The isoscalar-corrected ratio R_{A} / R_{D} for several nuclei (A) with respect to deuterium as a function of Q^{2} for four different x bins Aug 11, 2003 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-089 F2 f2ratio |
Ratio of isoscalar Born cross sections of inclusive deep-inelastic lepton scattering from nitrogen and deuterium for fixed values of x as a function of epsilon Aug 11, 2003 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-088 F2 f2ratio |
Ratio of isoscalar Born cross sections of inclusive deep-inelastic lepton scattering from nitrogen and deuterium for fixed values of x as a function of Q^{2} Aug 11, 2003 *BW (eps) *BW (pdf) *Data |
A. Bruell
final |
03-087 F2 f2ratio |
Ratio of isoscalar Born cross sections of inclusive deep-inelastic lepton scattering from nucleus A and D versus x Aug 11, 2003 *BW (eps) *BW (pdf) *Data |
A. Bruell
final |
03-086 F2 f2ratio |
Comparison between data (open and closed circles) and MC simulation (histogram) for the ratio of fractional changes in the yields of nitrogen and deuterium when treating the upper and lower HERMES detector halves independently Aug 11, 2003 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-085 F2 f2ratio |
Ratio of track reconstruction efficiencies in $^1$H, $^3$He, $^{14}$N and $^{84}$Kr with respect to $^2$H as function of $x$ Aug 11, 2003 *BW (eps) *BW (pdf) |
A. Bruell
final |
03-084 F2 f2ratio |
The nuclear-elastic Bethe-Heitler cross section on ^{14}N Aug 11, 2003 *BW (eps) *BW (pdf) |
A. Bruell
final |
97-008 G1 neutron |
A_{1}^{n} and g_{1}^{n} in comparison to E142 1997 *BW *BW (eps) *BW (pdf) |
A. Bruell
final |
96-104 CHARM general |
Plot of world data on photoproduction xsec for charm, with HERMES energy range highlighted in yellow Feb 3, 2000 *Colour (eps) *Colour (pdf) |
A. Bruell
final |
12-030 DVCS |
The beam-charge asymmetry amplitudes extracted in 4 and 6 bins Jul 6, 2012 *Colour (pdf) INFO: Supportive plot. INFO: The data values are contained in the file attached to the entry 12-029 |
J. Burns and M. Murray
final |
12-029 DVCS |
The beam-charge asymmetry amplitudes extracted in 4 and 6 bins Jul 6, 2012 *Colour (pdf) *Data INFO: Supportive plot. The data values are contained in the file attached to this entry |
J. Burns and M. Murray
final |
12-028 DVCS |
The covariance matrix results for the asymmetries extracted in a single bin across the whole kinematic range. The size of the symbols in the chart reflect the magnitude of the corresponding correlation. Closed (open) symbols represent positive (negative) correlations Jul 6, 2012 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to the entry 12-022 |
J. Burns and M. Murray
final |
12-027 DVCS |
The beam-charge asymmetry amplitudes extracted from all the unpolarised hydrogen data recorded at HERMES from 1996 until 2007 as a function of -t for three different x_{B} ranges. The error bars (bands) represent the statistical (systematic) uncertainties. The simulated fractional contribution from associated production to the yield in each kinematic bin is shown in the bottom row Jul 6, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 12-022 |
J. Burns and M. Murray
final |
12-026 DVCS |
The beam-helicity asymmetry amplitudes extracted from all the unpolarised hydrogen data recorded at HERMES from 1996 until 2007 as a function of -t for three different x_{B} ranges. The error bars (bands) represent the statistical (systematic) uncertainties. An additional 3.2 % scale uncertainty is present in the amplitudes due to the uncertainty of the beam polarisation measurement. The simulated fractional contribution from associated production to the yield in each kinematic bin is shown in the bottom row Jul 6, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 12-022 |
J. Burns and M. Murray
final |
12-025 DVCS |
The beam-charge asymmetry amplitudes extracted from all the unpolarised hydrogen data recorded at HERMES from 1996 until 2007. The error bars (bands) represent the statistical (systematic) uncertainties. Theoretical calculations are shown as solid and dashed lines (KM09) or as dashed-dotted lines (GGL11). See text for details. The simulated fractional contribution from associated production to the yield in each kinematic bin is shown in the bottom row Jul 6, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 12-022 |
J. Burns and M. Murray
final |
12-024 DVCS |
The beam-helicity asymmetry amplitudes extracted from all the unpolarised hydrogen data recorded at HERMES from 1996 until 2007. The error bars (bands) represent the statistical (systematic) uncertainties. An additional 3.2 % scale uncertainty is present in the amplitudes due to the uncertainty of the beam polarisation measurement. Solid, dashed (KM09) and dashed-dotted lines (GGL11) show model calculations. See text for details. The simulated fractional contribution from associated production to the yield in each kinematic bin is shown in the bottom row Jul 6, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 12-022 |
J. Burns and M. Murray
final |
12-023 DVCS |
Beam-charge asymmetry amplitudes extracted separately from the unpolarised 1996-2005 (open triangles) and 2006-2007 (filled squares) hydrogen data. The error bars represent the statistical uncertainties. The error bands represent the systematic uncertainties. The simulated fractional contribution from associated production to the yield in each kinematic bin is shown in the bottom row Jul 6, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 12-022 |
J. Burns and M. Murray
final |
12-022 DVCS |
Beam-helicity asymmetry amplitudes extracted separately from the unpolarised 1996-2005 (open triangles) and 2006-2007 (filled squares) hydrogen data. The error bars represent the statistical uncertainties. The error bands represent the systematic uncertainties. An additional 2.8 % and 3.4 % scale uncertainty for the 1996-2005 and 2006-2007 data respectively is present in the amplitudes due to the uncertainty of the beam polarisation measurement. The simulated fractional contribution from associated production to the yield in each kinematic bin is shown in the bottom row Jul 6, 2012 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry |
J. Burns and M. Murray
final |
12-021 DVCS |
The leading Bethe-Heitler process, i.e. the emission of a real photon from the incoming or outgoing lepton. This process has the same initial and final states as DVCS Jul 6, 2012 *Colour (pdf) |
J. Burns and M. Murray
final |
12-020 DVCS |
The leading DVCS process in which an electron/positron interacts with a quark in the nucleon via a virtual photon. The quark is found in the nucleon with longitudinal momentum fraction x+xi and emits a real photon. The quark is absorbed by the nucleon withlongitudinal momentum fraction x-xi Jul 6, 2012 *Colour (pdf) |
J. Burns and M. Murray
final |
Author: C | ||
Back to top | ||
96-056 EXPERIMENT spectrometer |
Mass Spectrum, O.4 to 1.2 GeV 1996 *Colour *Colour (eps) *Colour (pdf) |
P. Carter
final |
Author: D | ||
Back to top | ||
06-049 G1 |
Top two panels: measured and unfolded Born asymmetries for proton and deuteron. The error bars of the Born asymmetries are the square root of the diagonal elements of the covariance matrix obtained after unfolding, with the inclusion of the uncertainty due to the statistics of the Monte Carlo. Bottom panel: uncertainty inflation when going from measured to Born asymmetry due to the unfolding procedure. The symbols A, B and C refer to the Q^{2}-bins Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-048a G1 |
Migration matrices $M_{\spar}$ (the $M_{\sant}$ matrices look similar) for two different binnings. Migration matrix for a pure x binning. The horizontal and vertical lines divide the x-bins; within each x-bin the Q^{2}-bins are arranged in increasing Q^{2}. The matrices are extracted from a fully reconstructed Monte Carlo data set simulating both QED radiative and detector effects for inclusive DIS on a proton target Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-048b G1 |
Migration matrices $M_{\spar}$ (the $M_{\sant}$ matrices look similar) for two different binnings. Migration matrix for the combined x and Q^{2} binning used in this analysis. The horizontal and vertical lines divide the x-bins; within each x-bin the Q^{2}-bins are arranged in increasing Q^{2}. The matrices are extracted from a fully reconstructed Monte Carlo data set simulating both QED radiative and detector effects for inclusive DIS on a proton target Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-047 G1 |
Integrals of g_{1}^{p,d,n,NS} over the range 0.021= Oct 31, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
L. De Nardo
final |
06-046 G1 |
Top panel: xg_{1}^{n} from data for g_{1}^{p} and g_{1}^{d}. Bottom panel: the x-weighted non-singlet spin structure function xg_{1}^{NS}, compared to data from SMC, E143, and E155. All data are presented at their measured values of < Q^{2} >$, except that the E155 data in each x bin have been averaged over Q^{2} for visual purposes. Total uncertainties are shown as bars. For the HERMES data the closed (open) symbols represent values derived by selecting events with Q^{2} >1GeV^{2} (Q^{2}<1GeV^{2}) Oct 31, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
L. De Nardo
final |
06-046a G1 |
Same as 06-046 just with including a panel for Q^{2} vs x for the different experiments Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-045 G1 |
Top panel: the structure function g_{1}^{n} obtained from g_{1}^{p} and g_{1}^{d}, compared with similar data from SMC, E143, and E155 in the HERMES x-range. Second panel from the top: g_{1}^{n} as obtained from a He^{3} target by JLab, HERMES, E142, and E154. Total error bars are shown, obtained by combining statistical and systematic uncertainties in quadrature. The bottom panel shows the < Q^{2} >$ of each data point in the top two panels. E155 data have been averaged over their Q^{2} bins for visibility. For the HERMES data the closed (open) symbols represent values derived by selecting events with $Q^{2} >1$~GeV$^2$ ($ Q^{2} <1$~GeV$^2$) Oct 31, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
L. De Nardo
final |
06-045a G1 |
Same as 06-045 just xg_{1}^{n} Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-044 G1 |
HERMES results on xg_{1}^{p} and xg_{1}^{d} vs x, shown on separate panels, compared to data from SMC, E143, E155, and COMPASS. The error bars represent the sum in quadrature of statistical and systematic uncertainties. The HERMES data points shown are statistically correlated by unfolding QED radiative and detector smearing effects; the statistical uncertainties shown are obtained from only the diagonal elements of the covariance matrix. The E143 and E155 data points are correlated due to the method for correcting for QED radiation. For the HERMES data the closed (open) symbols represent values derived by selecting events with Q^{2}>1GeV^{2} (Q^{2} <1GeV^{2} ) Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-044a G1 |
Same plot as 06-044 just without Q^{2} pannel and the COMPASS data are from hep-ex/0609038 and not from hep-ex/0501073 like in the bw-paper plots Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-044b G1 |
Q^{2}-panel plot for 06-044a Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-043 G1 |
HERMES results for xg_{1} vs x for the proton and the deuteron. Error bars represent statistical uncertainties of the data (from the diagonal elements of the covariance matrix combined quadratically with those from Monte Carlo statistics. The upper and lower error bands represent the total systematic uncertainties for the proton and deuteron, respectively. The deuteron data points have been slightly shifted in x for visibility. The closed (open) symbols represent values derived by selecting events with Q^{2} >1GeV^{2} (Q^{2} <1GeV^{2}) Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-043a G1 |
same plot as 06-043 with Q^{2}-panel for the HERMES-points Oct 31, 2006 *Colour (eps) |
L. De Nardo
final |
06-042 G1 |
HERMES results on g_{1}^{p} and g_{1}^{d} vs x, shown on separate panels, compared to data from SMC, E143, E155, and COMPASS, in the HERMES x-range. Error bars represent the sum in quadrature of statistical and systematic uncertainties. The HERMES data points shown are statistically correlated by unfolding QED radiative and detector smearing effects; the statistical uncertainties shown are obtained from only the diagonal elements of the covariance matrix. The E143 and E155 data points are correlated through QED radiative corrections. The E155 points have been averaged over their $Q^{2}$ bins for visibility. For the HERMES data the closed (open) symbols represent values derived by selecting events with Q^{2} >1GeV^{2} (Q^{2} <1GeV^{2}) Oct 31, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) INFO: For the color plot the COMPASS data are from hep-ex/0609038 and not from hep-ex/0501073 like in the bw-paper plots |
L. De Nardo
final |
06-042a G1 |
Panel with Q^{2} vs x for the different experiments for plot 06-042 Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-041 G1 |
HERMES results on A_{1}^{p} and A_{1}^{d} vs x, shown on separate panels, compared to data from SMC, E143, E155, and COMPASS. Error bars represent the sum in quadrature of statistical and systematic uncertainties. For the HERMES data the closed (open) symbols represent values derived by selecting events with Q^{2} >1GeV^{2} (Q^{2} <1GeV^{2}). The HERMES data points shown are statistically correlated by unfolding QED radiative and detector smearing effects; the statistical uncertainties shown are obtained from the diagonal elements of the covariance matrix, only. The E143 and E155 data points are correlated through QED radiative corrections. The lower panel shows the x dependence of < Q^{2} >$ for the different experiments Oct 31, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) INFO: For the color plot the COMPASS data are from hep-ex/0609038 and not from hep-ex/0501073 like in the bw-paper plots |
L. De Nardo
final |
06-041a G1 |
Same as plot 06-041 just without Q^{2}-panel Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-041b G1 |
Panel with Q^{2} vs x for the different experiments for plot 06-041 Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-040 G1 |
HERMES results on A_{1} vs x for proton and deuteron. Error bars represent statistical uncertainties of the data (diagonal elements of the covariance matrix) combined quadratically with those from Monte Carlo statistics. Bands represent systematic uncertainties. Deuteron data points have been slightly shifted in $x$ for visual purposes Oct 31, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
L. De Nardo
final |
06-039 G1 |
Correlation matrix in 19 x-bins of g_{1} for the proton. The closed symbols represent positive values, while the open ones are for negative values. The area of the symbols represents the size of the correlation Oct 31, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
L. De Nardo
final |
06-039a G1 |
same as 06-039 just for deuterium Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-038 G1 |
Efficiency for the detection of B-H elastic (el.) and quasi-elastic (q.el.) events in the HERMES spectrometer, for scattering on both deuteron (d) and proton (p). The efficiency is set to unity for x>0.1 Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-037 G1 |
The distribution of events originating from the arbitrarily selected x-bin shown as a shaded area, from a simulation of QED radiative effects and detector smearing, using a proton target. The vertical lines indicate x-bin boundaries Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-036 G1 |
Percentage of charge symmetric background in each $x-Q^{2}$ bin, for the proton and the deuteron targets Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-035 G1 |
Kinematic x-Q^{2} and x-y planes covered by this analysis. The symbols represent the average values of (x,Q^{2}) (top panel) and (x,y) (bottom panel) in each bin. Subdivision of the x-bins along Q^{2} is denoted by different symbols (A, B, C) Oct 31, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
L. De Nardo
final |
06-035a G1 |
Kinematic x-y planes covered by this analysis. The symbols represent the average values (x,y) in each bin. Subdivision of the x-bins along Q^{2} is denoted by different symbols (A, B, C) Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-034 G1 |
A schematic side view of the HERMES spectrometer Oct 31, 2006 *Colour (eps) *Colour (pdf) |
L. De Nardo
final |
06-033 G1 |
Schematic view of the longitudinally polarized target. From left to right: Atomic Beam Source (ABS) containing Radio-Frequency Transitions (RFT), target chamber with cell and magnet, diagnostic system composed by Target Gas Analyzer (TGA), and Breit-Rabi Polarimeter (BRP) Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-032 G1 |
Schematic picture of Deep-Inelastic Scattering for one photon exchange Oct 31, 2006 *BW (eps) *BW (pdf) |
L. De Nardo
final |
06-032a G1 |
Tar-file including all the Hermes data included in the paper Oct 31, 2006 *Data |
L. De Nardo
final |
06-029 DIAGRAM |
Diagram of polarized semi-inclusive DIS for a logitudinal polarized target, showing a realistic view on fragmentation Jun 12, 2006 *Colour (eps) *Colour (pdf) *Colour (fig) |
B. Maiheu / L. de Nardo
final |
03-112 G1 |
First moments of polarized parton densities for Method 1 and 2 in LO and NLO at Q^{2} = 2.5 and 4.0 GeV^{2} calculated also for the measured x ranges (inclucive and semi-inclusive) Nov 18, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-111 G1 |
The polarized parton density xDelta_{Sigma}(x) at the input scale Q_{0}^{2} = 4.0 GeV^{2} (solid line) as resulting from Method 2. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are shown for comparison. The shaded area represent the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated Nov 18, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-110 G1 |
The polarized parton densitY xDelta_{Sigma}(x) at the input scale Q_{0}^{2} = 4.0 GeV^{2} (solid line) as resulting from Method 1. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are shown for comparison. The shaded area represent the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated Nov 18, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-109 G1 |
The polarized gluon density xDelta_{G}(x) at the input scale Q_{0}^{2} = 4.0 GeV^{2} (solid line) as resulting from Method 2. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are shown for comparison. The shaded area represents the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated Nov 18, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-108 G1 |
The polarized gluon density xDelta_{G}(x) at the input scale Q_{0}^{2} = 4.0 GeV^{2} (solid line) as resulting from Method 1. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are shown for comparison. The shaded area represents the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated Nov 18, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-107 G1 |
The polarized parton densities xDelta_{q}_nsp(x)$, xDelta_{q}_nsn(x), xDelta_{G}(x), and xDelta_{Sigma}(x) at the input scale Q_{0}^{2} = 4.0 GeV^{2} (solid line) as resulting from Method 2. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are shown for comparison. The shaded areas represent the fully correlated 1sigma statistical error bands Nov 18, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-106 G1 |
The polarized parton densities xDelta_{uv}(x), xDelta_{dv}(x), xDelta_{G}(x), and xDelta_{qbar}(x) at the input scale Q_{0}^{2} = 4.0 GeV^{2} (solid line) as resulting from Method 1. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are shown for comparison. The shaded areas represent the fully correlated $1\sigma$ statistical error bands. The dark dotted lines correspond to the positivity bounds taken from unpolarized densities (GRV98) Nov 18, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-022 G1 |
Differences in the choice of the parameterizations Feb 5, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-021 G1 |
Final parameter values and their statistical errors at the input scale of 4 GeV^{2} Feb 5, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-020 G1 |
The world data on xg1n(x) together with the NLO QCD curve (solid line) as resultng from Method 2. The experimental data are evolved to a common value of Q^{2} = 5.0 GeV^{2} (only the data points measured at Q^{2} > 1.0 GeV^{2} and entering the QCD fit are taken). The error bars shown are the statistical and systematic ones added in quadrature. The shaded area represents the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are drawn for comparison Nov 18, 2003 *Colour (eps) |
L. De Nardo and H. Boettcher
prelim |
03-019 G1 |
The world data on xg1d(x) together with the NLO QCD curve (solid line) as resulting from Method 2. The experimental data are evolved to a common value of Q^{2} = 5.0 GeV^{2} (only the data points measured at Q^{2} > 1.0 GeV^{2} and entering the QCD fit are taken). The error bars shown are the statistical and systematic ones added in quadrature. The shaded area represents the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are drawn for comparison Nov 18, 2003 *Colour (eps) |
L. De Nardo and H. Boettcher
prelim |
03-018 G1 |
The world data on xg1p(x) together with the NLO QCD curve (solid line) as resulting from Meyhod 2. The experimental data are evolved to a common value of Q^{2} = 5.0 GeV^{2} (only the data points measured at Q^{2} > 1.0 GeV^{2} and entering the QCD fit are taken). The error bars shown are the statistical and systematic ones added in quadrature. The shaded area represents the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are drawn for comparison Nov 18, 2003 *Colour (eps) |
L. De Nardo and H. Boettcher
prelim |
03-017 G1 |
The world data on xg1n(x) together with the NLO QCD curve (solid line) as resulting from Method 1. The experimental data are evolved to a common value of Q^{2} = 5.0 GeV^{2} (only the data points measured at Q^{2} > 1.0 GeV^{2} and entering the QCD fit are taken). The error bars shown are the statistical and systematic ones added in quadrature. The shaded area represents the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are drawn for comparison Nov 18, 2003 *Colour (eps) |
L. De Nardo and H. Boettcher
prelim |
03-016 G1 |
The world data on xg1d(x) together with the NLO QCD curve (solid line) as resulting from Method 1. The experimental data are evolved to a common value of Q^{2} = 5.0 GeV^{2} (only the data points measured at Q^{2} > 1.0 GeV^{2} and entering the QCD fit are taken). The error bars shown are the statistical and systematic ones added in quadrature. The shaded area represents the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are drawn for comparison Nov 18, 2003 *Colour (eps) |
L. De Nardo and H. Boettcher
prelim |
03-015 G1 |
The world data on xg1p(x) together with the NLO QCD curve (solid line) as resulting from Method 1. The experimental data are evolved to a common value of Q^{2} = 5.0 GeV^{2} (only the data points measured at Q^{2} > 1.0 GeV^{2} and entering the QCD fit are taken). The error bars shown are the statistical and systematic ones added in quadrature. The shaded area represents the fully correlated 1sigma statistical error band. The hatched areas are the systematic uncertainties as indicated. The results obtained by BB (long--dashed line), GRSV (dashed--dotted line), and AAC (dashed line) are drawn for comparison Nov 18, 2003 *Colour (eps) |
L. De Nardo and H. Boettcher
prelim |
03-014 G1 |
Comparison of the central curves for xg1p, xg1d, and xg1n at Q^{2}= 4 GeV^{2} as resulting from Method 1 and 2, with inserts showing the high-x region Feb 5, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-013 G1 |
Comparison of the fully correlated 1sigma statistical error bands for xg1p, xg1d, and xg1n at Q^{2}=4 GeV^{2} as resulting from Method 1 and 2 Feb 5, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-012 G1 |
Same as fig4, but with the systematic bands from Method 2 Feb 5, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-011 G1 |
Fully correlated 1sigma statistical error bands for the polarized gluon distributions extracted by Method 1 and 2, together with the systematic uncertainties determined from Method 1. The dark solid line represents the positivity limit as taken from the GRV fit Feb 5, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
03-010 G1 |
Comparison of the fully correlated 1sigma statistical error bands for the singlet and non-singlet distributions at Q^{2}=4 GeV^{2} as resulting from Method 1 and 2 Feb 5, 2003 *Colour (eps) *Colour (pdf) |
L. De Nardo and H. Boettcher
prelim |
06-011 HYPERONS lambda |
The L(1520) to pK- invariant mass spectrum with unbinned fit results. The obtained mass value has been corrected for acceptance effects 2006 *Colour (eps) *Colour (pdf) INFO: supportive plot for the partial cross section for P>6GeV of the Lambda(1520) (with Pz > 6.0 GeV) = 65.3 +/- 8.8 (stat) +/- 6.9 (syst) nb. SEE 06-010 for the syst. uncertainty. |
W. Deconinck, S. Wang
prelim |
06-010 HYPERONS lambda |
The L-bar(1520) to p-bar K^{+} invariant mass spectrum with unbinned fit results. The obtained mass value has been corrected for acceptance effects 2006 *Colour (eps) *Colour (pdf) INFO: supportive plot for the partial cross section for P>6GeV of the anti-Lambda(1520) (with Pz > 6.0 GeV) = 9.8 +/- 2.6 (stat) +/- 0.9 (syst) nb and the ratio anti-Lambda(1520)/Lambda(1520)= 0.15 +/- 0.05 (stat) +/- 0.02 (syst). Particle and anti-particle are assumed to be produced unpolarised. The systematic uncertainty in the cross section ratio is obtained from the variation in the signal counts when varying the fits for the mass peaks within the total uncertainty of the determined mass. |
W. Deconinck, S. Wang
prelim |
05-108 EXOTICS pentaquark |
K^{0}_{s} spectrum associated with Theta-bar spectrum Jul 28, 2005 *Colour (eps) *Colour (pdf) |
W. Deconinck
prelim |
05-107 EXOTICS pentaquark |
The Theta-bar spectrum Jul 28, 2005 *Colour (eps) *Colour (pdf) |
W. Deconinck
prelim |
05-069 EXOTICS pentaquark |
schematic plot show the decay topology and the placed cuts for the Xi-- 2005 *Colour (eps) *Colour (pdf) *Colour (fig) |
W. Deconinck
final |
01-021 FRAGMENTATION pion |
Total (neutral plus charged) pion multiplicity as a function of Q^{2} for various z-bins. The systematic uncertainty on the data is 8.5percent. The three curves shown are NLO QCD calculations of fragmentation functions (see paper) Mar 20, 2001 *BW (eps) *BW (pdf) *Data |
P. Di Nezza
final |
01-020 FRAGMENTATION pion |
Charged pion multiplicities from HERMES (filled symbols) as a function of x in four different z-bins, compared to charged hadron multiplicities from EMC (open symbols). All data have been evolved to 2.5~GeV^{2} and are plotted at the measured x-value Mar 20, 2001 *BW (eps) *BW (pdf) *Data |
P. Di Nezza
final |
01-019 FRAGMENTATION pion |
Multiplicities for charged pions (note the EMC data for charged pions are for fragmentation functions). The HERMES results have been evolved to Q^{2}=25 GeV^{2} using a NLO QCD model. Only statistical uncertainties are shown. The systematic uncertainties for neutral pions are 7percent for HERMES and less than or equal 10percent for EMC Mar 20, 2001 *BW (eps) *BW (pdf) *Data |
P. Di Nezza
final |
01-018 FRAGMENTATION pion |
Multiplicities for neutral pions. The HERMES results have been evolved to Q^{2}=25 GeV^{2} using a NLO QCD model. Only statistical uncertainties are shown. The systematic uncertainties for neutral pions are 9percent for HERMES and less than or equal 13percent for EMC Mar 20, 2001 *BW (eps) *BW (pdf) *Data |
P. Di Nezza
final |
01-017 FRAGMENTATION pion |
Average charged pion multiplicity from HERMES compared to EMC fragmentation functions. Only the statistical uncertainties are s hown. The systematic uncertainties for neutral (charged) pions are 9percent (7percent) for HERMES, less than or equal 15percent for SLAC and less than or equal 13percent (10percent) for EMC Mar 20, 2001 *BW (eps) *BW (pdf) |
P. Di Nezza
final |
01-016 FRAGMENTATION pion |
pi^{0} multiplicity from HERMES, EMC and SLAC Mar 20, 2001 *BW (eps) *BW (pdf) |
P. Di Nezza
final |
01-015 FRAGMENTATION pion |
Ratio of neutral to average charged pion multiplicities. The systematic uncertainty on the ratio (not included in the error bar) is 6percent Mar 20, 2001 *BW (eps) *BW (pdf) |
P. Di Nezza
final |
01-014 FRAGMENTATION pion |
Neutral (circles) and average charged (triangles) pion multiplicities. The error bars show the statistical uncertainty only. The systematic uncertainty for the charged (neutral) pions is 7percent (9percent). The solid line is a parameterization using the independent fragmentation model. The dashed line is a fit to the present neutral pion data using the parameterization given in the text. The charged pion data have been shifted slightly in z to make them visible Mar 20, 2001 *BW (eps) *BW (pdf) *Data |
P. Di Nezza
final |
01-013 FRAGMENTATION pion |
Detection probability as a function of z for charged (triangles) and neutral (circles) pions when the DIS positron is detected Mar 20, 2001 *BW (eps) *BW (pdf) |
P. Di Nezza
final |
01-012 FRAGMENTATION pion |
Comparison between the measured and simulated pion energy spectra. Filled circles (triangles) are the neutral (charged) pion measurements. The histograms are the simulated spectra for neutral (dashed line) and charged (full line) pions. All spectra have been normalized to unit area Mar 20, 2001 *BW (eps) *BW (pdf) |
P. Di Nezza
final |
01-011 FRAGMENTATION pion |
Two-photon invariant mass spectrum. The solid line is a fit with a Gaussian plus a polynomial. The dashed line represents the background only Mar 20, 2001 *BW (eps) *BW (pdf) |
P. Di Nezza
final |
01-010 FRAGMENTATION pion |
Semi-inclusive pion electroproduction diagram Mar 20, 2001 *BW (eps) *BW (pdf) |
P. Di Nezza
final |
11-007 TRANSVERSE |
The 2 < cos(2phi-phi_{s}) > _LT azimuthal amplitude of the asymmetry for pions and kaons as a function of x, z or Ph\perp. The systematic uncertainty is given as a band at the bottom of each panel. In addition there is a 8% scale uncertainty from the accuracy in the measurements of the target and beam polarizations Apr 20, 2011 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
11-006 TRANSVERSE |
The 2 < cos(phi-phi_{s}) > _LT azimuthal amplitude of the asymmetry for pions and kaons as a function of x, z or Ph\perp. The systematic uncertainty is given as a band at the bottom of each panel. In addition there is a 8% scale uncertainty from the accuracy in the measurements of the target and beam polarizations Apr 20, 2011 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
11-005 TRANSVERSE |
The 2 < cos(phi_{s}) > _LT azimuthal amplitude of the asymmetry for pions and kaons as a function of x, z or Ph\perp. The systematic uncertainty is given as a band at the bottom of each panel. In addition there is a 8% scale uncertainty from the accuracy in the measurements of the target and beam polarizations Apr 20, 2011 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
09-063 TRANSVERSE |
sin(3phi-phi_{S}) amplitudes of the A_{UT} asymmetry for semi-inclusive pions (+, -, or 0) and kaons (+ or -) as a function of x, z, or P_{h\perb}. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-062 TRANSVERSE |
The same as entry 09-063, but only for pions Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-061 TRANSVERSE |
The same as entry 09-063, but only for kaons Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-060 TRANSVERSE |
sin(phi_{S}) amplitudes of the A_{UT} asymmetry for semi-inclusive pions (+, -, or 0) and kaons (+ or -) as a function of x, z, or P_{h\perb}. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-059 TRANSVERSE |
The same as entry 09-060, but only for pions Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-058 TRANSVERSE |
The same as entry 09-060, but only for kaons Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-057 TRANSVERSE |
sin(phi_{S}) amplitude of the A_{UT} asymmetry for semi-inclusive pions (-) as a function of x, for 2 different Q^{2} ranges in each of the x-bins: one above and one below the average Q^{2} in the bin. The lower panel gives the respective average Q^{2}. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-056 TRANSVERSE |
sin(2phi-phi_{S}) amplitudes of the A_{UT} asymmetry for semi-inclusive pions (+, -, or 0) and kaons (+ or -) as a function of x, z, or P_{h\perb}. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-055 TRANSVERSE |
The same as entry 09-056, but only for pions Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-054 TRANSVERSE |
The same as entry 09-056, but only for kaons Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-053 TRANSVERSE |
sin(2phi+phi_{S}) amplitudes of the A_{UT} asymmetry for semi-inclusive pions (+, -, or 0) and kaons (+ or -) as a function of x, z, or P_{h\perb}. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-052 TRANSVERSE |
The same as entry 09-053, but only for pions Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-051 TRANSVERSE |
The same as entry 09-053, but only for kaons Oct 20, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-063. |
M. Diefenthaler, A. Rostomyan, G. Schnell, M. Contalbrigo, L. Pappalardo
prelim |
09-050 TRANSVERSE sivers |
Sivers amplitudes for pions, charged kaons, and the pion-difference asymmetry in bins of x, z, and P_{h,perb}. The systematic uncertainty is given as a band at the bottom of each panel. In addition, there is a 7.3% scale uncertainty from the target-polarization measurement. Full 2002-2005 transverse data set Aug 4, 2009 *BW (eps) *BW (pdf) *Data INFO: The data are contained in the file attached to this entry. |
M. Diefenthaler and L. Pappalardo
final |
09-050a TRANSVERSE sivers |
Same as entry 09-050, but only for pions and in color for presentations Aug 4, 2009 *Colour (eps) *Colour (pdf) INFO: The data are contained in the file attached to entry 09-050. |
M. Diefenthaler and L. Pappalardo
final |
09-050b TRANSVERSE sivers |
Same as entry 09-050, but only for kaons and in color for presentations Aug 4, 2009 *Colour (eps) *Colour (pdf) INFO: The data are contained in the file attached to entry 09-050. |
M. Diefenthaler and L. Pappalardo
final |
09-050c TRANSVERSE sivers |
Same as entry 09-050, but only for the pion difference asymmetry (+ minus -) and in color for presentations Aug 4, 2009 *Colour (eps) *Colour (pdf) INFO: The data are contained in the file attached to entry 09-050. |
M. Diefenthaler and L. Pappalardo
final |
09-049a TRANSVERSE sivers |
Sivers amplitudes for positively charged pions as functions of z or P_{h,perb}, compared for two different ranges in Q^{2}. The corresponding fraction of pions stemming from the decay of exclusive vector mesons is provided in the bottom panel (MC) Aug 4, 2009 *Colour (eps) *Colour (pdf) *Data INFO: The data are contained in the file attached to this entry. |
M. Diefenthaler and L. Pappalardo
final |
09-049b TRANSVERSE sivers |
As 09-049a, but for positively charged kaons Aug 4, 2009 *Colour (eps) *Colour (pdf) INFO: The data are contained in the file attached to entry 09-049a |
M. Diefenthaler and L. Pappalardo
final |
09-048a TRANSVERSE sivers |
Sivers amplitudes for positively charged pions as functions of x. The Q^{2} range for each bin was divided into the two regions above and below the average Q^{2} of each x-bin. In the bottom panel, the average Q^{2} values are given for the two Q^{2} ranges Aug 4, 2009 *Colour (eps) *Colour (pdf) *Data INFO: The data are contained in the file attached to this entry. |
M. Diefenthaler and L. Pappalardo
final |
09-048b TRANSVERSE sivers |
As 09-048a, but for positively charged kaons Aug 4, 2009 *Colour (eps) *Colour (pdf) INFO: The data are contained in the file attached to entry 09-048a |
M. Diefenthaler and L. Pappalardo
final |
09-047 TRANSVERSE sivers |
Difference of Sivers amplitudes for positively charged pions and positively charged kaons as function of x for all Q^{2}, and separated into the high- and low-Q^{2} regions as done for 09-048 Aug 4, 2009 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data INFO: The data are contained in the file attached to this entry. |
M. Diefenthaler and L. Pappalardo
final |
07-043 TRANSVERSE |
Collins moments of A_{UT} for pi^{+} and pi^{-} production overlaid with model calculation of Schweitzer et al (hep-ph/0603054) Feb 7, 2008 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
07-040 TRANSVERSE |
Collins moments of A_{UT} for pi^{+}, pi^{-}, and pi^{0} production (overlaid) from the full 2002-2005 data Feb 7, 2008 *Colour (eps) *Colour (pdf) INFO: See records 07-008 and 07-009 for data tables. |
M. Diefenthaler and L. Pappalardo
prelim |
07-039 TRANSVERSE |
Collins moments of A_{UT} for pi^{+}, pi^{-}, and pi^{0} production (in separate panels) from the full 2002-2005 data Feb 7, 2008 *Colour (eps) *Colour (pdf) INFO: See records 07-008 and 07-009 for data tables. |
M. Diefenthaler and L. Pappalardo
prelim |
07-015 TRANSVERSE |
Sivers moments of A_{UT} for pi^{+} and K^{+} (overlaid) and pi^{-} and K^{-} (overlaid) production from the full 2002-2005 data May 29, 2007 *Colour (eps) *Colour (pdf) INFO: See records 07-012 and 07-014 for data tables. |
M. Diefenthaler and L. Pappalardo
prelim |
07-014 TRANSVERSE |
Sivers moments of A_{UT} for SIDIS K^{+} and K^{-} production from the full 2002-2005 data May 29, 2007 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
07-013 TRANSVERSE |
Sivers moments of A_{UT} for pi^{0} production from the full 2002-2005 data May 29, 2007 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
07-012 TRANSVERSE |
Sivers moments of A_{UT} for SIDIS pi^{+} and pi^{-} production from the full 2002-2005 data May 29, 2007 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
07-011 TRANSVERSE |
Collins moments of A_{UT} for pi^{+} and K^{+} (overlaid) and pi^{-} and K^{-} (overlaid) production from the full 2002-2005 data May 29, 2007 *Colour (eps) *Colour (pdf) INFO: See records 07-008 and 07-010 for data tables. |
M. Diefenthaler and L. Pappalardo
prelim |
07-010 TRANSVERSE |
Collins moments of A_{UT} for SIDIS K^{+} and K^{-} production from the full 2002-2005 data May 29, 2007 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
07-009 TRANSVERSE |
Collins moments of A_{UT} for pi^{0} production from the full 2002-2005 data May 29, 2007 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
07-008 TRANSVERSE |
Collins moments of A_{UT} for SIDIS pi^{+} and pi^{-} production from the full 2002-2005 data May 29, 2007 *Colour (eps) *Colour (pdf) |
M. Diefenthaler and L. Pappalardo
prelim |
06-028 TRANSVERSE |
Sivers moments for charged pions and kaons as function of x, z and $P_{h\perp}$. The error band represents the systematic uncertainty of the kaons as described in 06-005 2006 *Colour (eps) *Colour (pdf) INFO: supportive plot; Please regard our latest plots with the full available statistics 07-015 |
M. Diefenthaler
prelim |
06-027 TRANSVERSE |
Virtual photon Collins moments for charged pions and kaons as function of x, z and $P_{h\perp}$. The error band represents the systematic uncertainty of the kaons as described in 06-005 2006 *Colour (eps) *Colour (pdf) INFO: supportive plot; supportive plot; Please regard our latest plots with the full available statistics 07-011 |
M. Diefenthaler
prelim |
06-014 TRANSVERSE |
Virtual photon Collins moments for charged pions as function of x, z and $P_{h\perp}$ compared to theoretical curves from [Efremov et al. hep-ph/0603054]. For the x-dependence the data are fitted using always a gaussian ansatz and a cQSM for the transversity function from [PRD64(2001),034013] to obtain a value for the favoured and unfavoured Collins ff (Eqn. 10 and 11 in hep-ph/0603054). In contrast, for the z dependence the curves are based on a fit of the Collins ff to the BELLE data and on the same cQSModel for the transversity function. The light shaded area indicates the sensitivity of the SSA to the unknown ratio of the gaussian width of h1 and H1^\perp 2006 *Colour (eps) *Colour (pdf) INFO: supportive plot; supportive plot; Please regard our latest plots with the full available statistics 07-008 |
M. Diefenthaler
prelim |
06-013 TRANSVERSE |
Sivers moments for charged pions as function of x, z and $P_{h\perp}$ compared to the results of a fit to our data by Anselmino et al. in PRD72,94007 using a certain parametrisation of the sivers function. The shaded area corresponds to the theoretical uncertainty due to the parameter errors (the 1-sigma deviation calculated from the parameter errors and their correlation matrices) 2006 *Colour (eps) *Colour (pdf) INFO: supportive plot; Please regard our latest plots with the full available statistics 07-012 |
M. Diefenthaler
prelim |
06-012 TRANSVERSE |
Sivers moments for charged kaons as function of x, z and $P_{h\perp}$ compared to the predictions of Anselmino et al. in PRD72,94007 obtained from fixing the parameters for the ansatz for the sivers function by fitting our pion data. The shaded area corresponds to the theoretical uncertainty due to the parameter errors 2006 *Colour (eps) *Colour (pdf) INFO: supportive plot; Please regard our latest plots with the full available statistics 07-014 |
M. Diefenthaler
prelim |
06-006 TRANSVERSE |
The contribution of vector mesons in the SIDIS Kaon sample 2006 *Colour (eps) *Colour (pdf) INFO: supportive plot |
M. Diefenthaler, U. Elschenbroich
prelim |
06-005 TRANSVERSE |
Sivers moments for charged kaons as function of x, z and $P_{h\perp}$. The error band represents the maximal systematic uncertainty due to RICH unfolding, acceptance and detector smearing effects and due to a possible contribution from the $\cos\phi$ moment in the unpolarised cross section. The common overall scaling uncertainty is due to the target polarisation uncertainty. The average values of the asymmetry and the kinematics are for K^{+}: A=0.0925+/-0.0147+/-0.0091, x=0.101, z=0.37, Pt=0.42, y=0.51, Q^{2}=2.51$ and for K^{-}: A=0.0167+/-0.0266+/-0.0093, x=0.096, z=0.33, Pt=0.39, y=0.52, Q^{2}=2.40 2006 *Colour (eps) *Colour (pdf) INFO: Please regard our latest plots with the full available statistics 07-014 |
M. Diefenthaler, U. Elschenbroich
prelim |
06-004 TRANSVERSE |
Virtual photon Collins moments for charged kaons as function of x, z and $P_{h\perp}$. The error band represents the uncertainties as in 06-005. The average values of the asymmetry are K^{+}: A=0.0172+/-0.0232+/-0.0177 and K^{-}: A=0.0605+/-0.0450+/-0.0220 and for the kinematics the same as given in 06-005 2006 *Colour (eps) *Colour (pdf) INFO: Please regard our latest plots with the full available statistics 07-010 |
M. Diefenthaler, U. Elschenbroich
prelim |
06-003 TRANSVERSE |
Lepton beam Collins moments for charged kaons as function of x, z and $P_{h\perp}$. The error band represents the uncertainties as in 06-005. The average values of the asymmetry are K^{+}: A=0.0059+/-0.0154+/-0.0078 and K^{-}: A=0.0502+/-0.0299+/-0.0146 and for the kinematics the same as given in 06-005 2006 *Colour (eps) *Colour (pdf) INFO: Please regard our latest plots with the full available statistics 07-010 |
M. Diefenthaler, U. Elschenbroich
prelim |
05-078 TRANSVERSE |
Lepton beam Collins moments as function of x, z and $P_{h\perp}$ for charged pions. The error band represents the maximal systematic uncertainty due to acceptance and detector smearing effects and due to a possible contribution from the $\cos\phi$ moment in the unpolarised cross section. The common overall scaling uncertainty is due to the target polarisation uncertainty. The average values of the asymmetry and the kinematics are for pi^{+}: A=0.020+/-0.0046+/-0.0012, x=0.095, z=0.36, Pt=0.40, y=0.54, Q^{2}=2.43 and for pi^{-}: A=-0.0254+/-0.0053+/-0.0015, x=0.091, z=0.35, Pt=0.40, y=0.54, Q^{2}=2.35 2005 *Colour (eps) *Colour (pdf) INFO: Please regard our latest plots with the full available statistics 07-008 |
M. Diefenthaler, U. Elschenbroich
prelim |
05-077 TRANSVERSE |
Virtual photon Collins moments as function of x, z and $P_{h\perp}$. The error band represents the maximal systematic uncertainty due to acceptance and detector smearing effects and due to a possible contribution from the $\cos\phi$ moment in the unpolarised cross section. The common overall scaling uncertainty is due to the target polarisation uncertainty. The average values of the asymmetry are pi^{+}: A=0.0373+/-0.0075+/-0.0018 and pi^{-}: A=-0.0423+/-0.0089+/-0.0024 and for the kinematics the same as given in 05-078 2005 *Colour (eps) *Colour (pdf) INFO: Please regard our latest plots with the full available statistics 07-008 |
M. Diefenthaler, U. Elschenbroich
prelim |
05-076 TRANSVERSE |
Sivers moments as function of x, z and $P_{h\perp}$. The error band represents the maximal systematic uncertainty due to acceptance and detector smearing effects and due to a possible contribution from the $\cos\phi$ moment in the unpolarised cross section. The common overall scaling uncertainty is due to the target polarisation uncertainty. The average values of the asymmetry are pi^{+}: A=0.0416+/-0.0046+/-0.0021 and pi^{-}: A=0.0030+/-0.0055+/-0.0007 and for the kinematics the same as given in 05-078 2005 *Colour (eps) *Colour (pdf) INFO: Please regard our latest plots with the full available statistics 07-012 |
M. Diefenthaler, U. Elschenbroich
prelim |
05-073 TRANSVERSE |
Dilution due to pions from exclusive vector meson production in the semi-inclusive pion sample for a proton target 2005 *Colour (eps) *Colour (pdf) INFO: supportive plot |
M. Diefenthaler, U. Elschenbroich
prelim |
05-118 HADRON-ATTENUATION |
The ratio $R_{2h}$ as a function of z_{2} for N^{14} (squares), Kr (circles) and Xe (triangles) with z_{1}>0.5 for Selection II. The systematic uncertainty is 4\% (3\%) for xenon and krypton (nitrogen) and is independent of z_{2}. The curves N^{14}: solid; Kr: dashed; Xe: dotted) are from the models by X.N.Wang and A.Majumder Oct 11, 2005 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
P. DiNezza
final |
05-117 HADRON-ATTENUATION |
The ratio $R_{2h}$ as a function of z_{2} for N^{14} (squares), Kr (circles) and Xe (triangles) with z_{1}>0.5. The systematical uncertainty is 2\% for all the targets and is independent of z_{2}. In the upper panel the curves (solid for N^{14}, dashed for Kr, dotted for Xe) are calculated within a BUU transport model by Falter et al. In the bottom panel the same data are shown with calculations that assume only absorption for the three nuclei (same line types as in the upper plot) Oct 11, 2005 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
P. DiNezza
final |
04-022 EXOTICS pentaquark |
nice plot show ing the production of pentaquarks 2004 *Colour (eps) *Colour (jpeg) *Colour (pdf) |
P. DiNezza
final |
01-123 DIAGRAM |
Illustrative plot of semi-inclusive scattering Sep 19, 2001 *Colour (eps) *Colour (pdf) |
M. Dueren
final |
01-112 DIAGRAM |
Illustrative plot of Delta-G measurement via a pair of high p_{T} hadrons Sep 19, 2001 *Colour (eps) *Colour (pdf) |
M. Dueren
final |
01-111 DIAGRAM |
Illustrative plot of proton spin puzzle Sep 19, 2001 *Colour (eps) *Colour (pdf) |
M. Dueren
final |
96-050 EXPERIMENT tracking |
Event display (high multiplicity event with 6 tracks and K^{0}_{s} in final state) 1996 *Colour (eps) *Colour (pdf) |
M. Dueren
final |
96-012 DIAGRAM |
Diagram of polarized semi-inclusive DIS 1996 *Colour (eps) *Colour (pdf) |
M. Dueren
final |
Author: E | ||
Back to top | ||
03-031 HADRON-ATTENUATION |
Q^{2} dependence of nuclear attenuation for pi^{+} and pi^{-} on ^{20}Ne target for different nu bins Apr 4, 2003 *Colour (eps) *Colour (pdf) |
G. Elbakian
prelim |
03-030 HADRON-ATTENUATION |
nu and z dependences of nuclear attenuation for protons and anti-protons produced from ^{4}He, ^{20}Ne and ^{84}Kr targets. The open triangles for the ^{84}Kr target correspond to extended kinematics with nu > 4 GeV and z > 0.1; the closed triangles are old released data for ^{84}Kr at nu > 7 GeV and z > 0.2 Apr 4, 2003 *Colour (eps) *Colour (pdf) |
G. Elbakian
prelim |
03-029 HADRON-ATTENUATION |
nu and z dependences of nuclear attenuation for K^{+} and K^{-} produced from ^{4}He, ^{20}Ne and ^{84}Kr targets. The open triangles for the ^{84}Kr target correspond to extended kinematics with nu > 2 GeV and z > 0.1; the closed triangles are old released data for ^{84}Kr at nu > 7 GeV and z > 0.2 Apr 4, 2003 *Colour (eps) *Colour (pdf) |
G. Elbakian
prelim |
03-028 HADRON-ATTENUATION |
nu and z dependences of nuclear attenuation for pi^{+} and pi^{-} produced from ^{4}He, ^{20}Ne and ^{84}Kr targets. The open triangles for the ^{84}Kr target correspond to extended kinematics with nu > 2 GeV and z > 0.1; the closed triangles are old released data for ^{84}Kr at nu > 7 GeV and z > 0.2 Apr 4, 2003 *Colour (eps) *Colour (pdf) |
G. Elbakian
prelim |
11-090a HADRON-ATTENUATION |
Dependence of R^{h}_{A} on z for positively charged hadrons for three slices in p_{t}^{2}. The inner and outer error bars indicate the statistical and total uncertainties, respectively. For the latter the statistical and systematic bin-to-bin uncertainties were added in quadrature. In addition, scale uncertainties of 3%, 5%, 4%, and 10% are to be considered for pions, kaons, protons and antiprotons, respectively Oct 26, 2011 *Colour (eps) *Colour (pdf) |
G. Elbakyan, N. Akopov
final |
11-090b HADRON-ATTENUATION |
Dependence of R^{h}_{A} on z for negatively charged hadrons for three slices in p_{t}^{2}. The inner and outer error bars indicate the statistical and total uncertainties, respectively. For the latter the statistical and systematic bin-to-bin uncertainties were added in quadrature. In a201012_{Helamprho}/data_{filesddition}, scale uncertainties of 3%, 5%, 4%, and 10% are to be considered for pions, kaons, protons and antiprotons, respectively Oct 26, 2011 *Colour (eps) *Colour (pdf) |
G. Elbakyan, N. Akopov
final |
11-089 HADRON-ATTENUATION |
Dependence of R^{h}_{A} on p_{t}^{2} for positively charged hadrons for three slices in z. The inner and outer error bars indicate the statistical and total uncertainties, respectively. For the latter the statistical and systematic bin-to-bin uncertainties were added in quadrature. In addition, scale uncertainties of 3%, 5%, 4%, and 10% are to be considered for pions, kaons, protons and antiprotons, respectively Oct 26, 2011 *Colour (eps) *Colour (pdf) |
G. Elbakyan, N. Akopov
final |
11-088a HADRON-ATTENUATION |
Dependence of R^{h}_{A} on z for positively charged hadrons for three slices in nu. The inner and outer error bars indicate the statistical and total uncertainties, respectively. For the latter the statistical and systematic bin-to-bin uncertainties were added in quadrature. In addition, scale uncertainties of 3%, 5%, 4%, and 10% are to be considered for pions, kaons, protons and antiprotons, respectively Oct 26, 2011 *Colour (eps) *Colour (pdf) |
G. Elbakyan, N. Akopov
final |
11-088b HADRON-ATTENUATION |
Dependence of R^{h}_{A} on z for negatively charged hadrons for three slices in nu. The inner and outer error bars indicate the statistical and total uncertainties, respectively. For the latter the statistical and systematic bin-to-bin uncertainties were added in quadrature. In addition, scale uncertainties of 3%, 5%, 4%, and 10% are to be considered for pions, kaons, protons and antiprotons, respectively Oct 26, 2011 *Colour (eps) *Colour (pdf) |
G. Elbakyan, N. Akopov
final |
11-087a HADRON-ATTENUATION |
Dependence of R^{h}_{A} on nu for positively charged hadrons for three slices in z. The inner and outer error bars indicate the statistical and total uncertainties, respectively. For the latter the statistical and systematic bin-to-bin uncertainties were added in quadrature. In addition, scale uncertainties of 3%, 5%, 4%, and 10% are to be considered for pions, kaons, protons and antiprotons, respectively Oct 26, 2011 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
G. Elbakyan, N. Akopov
final |
11-087b HADRON-ATTENUATION |
Dependence of R^{h}_{A} on nu for negatively charged hadrons for three slices in z. The inner and outer error bars indicate the statistical and total uncertainties, respectively. For the latter the statistical and systematic bin-to-bin uncertainties were added in quadrature. In addition, scale uncertainties of 3%, 5%, 4%, and 10% are to be considered for pions, kaons, protons and antiprotons, respectively Oct 26, 2011 *Colour (eps) *Colour (pdf) |
G. Elbakyan, N. Akopov
final |
06-020 DVCS proton |
The $cos \phi$ amplitude of the beam--charge asymmetry as a function of $-t$ for the exclusive region (-1.5GeV < M_{X} < 1.7GeV), after background correction. The error bars (band) represent(s) the statistical (systematic) uncertainties. The calculations based on GPD models (VGG, PRD 60 (1999) 094017, Goeke et al. Prog. Part. Nucl. Phys. 47 (2001) 401) use either a factorized t--dependence with (dashed--dotted) or without (dotted) the D-term contribution, or a Regge--inspired t--dependence with (dashed) or without (solid) the D-term contribution May 25, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
F. Ellinghaus
final |
06-019 DVCS proton |
function of the missing mass. Statistical uncertainties are shown May 25, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
F. Ellinghaus
final |
06-018 DVCS proton |
Beam--charge asymmetry $A_{C}$ for the hard electroproduction of photons off protons as a function of the azimuthal angle \phi, for the exclusive sample (-1.5GeV < M_{X} < 1.7GeV) before background correction. Statistical uncertainties are shown. The solid curve shows the result of a four--parameter fit: (-0.011\pm0.019) + (0.060\pm0.027) \cos \phi + (0.016\pm0.026) \cos 2 \phi + (0.034\pm0.027) \cos 3 \phi. The dashed line shows the pure \cos \phi dependence May 25, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
F. Ellinghaus
final |
06-017 DVCS proton |
Distributions in missing--mass squared from data (statistical error bars) and from Monte Carlo simulations (line). The latter include elastic BH (filled area) and associated BH (hatched area) processes as well as semi--inclusive background. The vertical lines enclose the selected exclusive region May 25, 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
F. Ellinghaus
final |
05-099 DVCS |
Missing Mass spectrum showing the exclusive and the semi-inclusive area. The different backgrounds leaking into the exclusive region are explained Jul 24, 2005 *Colour (eps) *Colour (pdf) |
F. Ellinghaus
prelim |
05-099a DVCS |
Missing Mass spectrum showing the exclusive and the semi-inclusive area. The different backgrounds leaking into the exclusive region are explained. Only the upper plot of 05-099 Jul 24, 2005 *Colour (eps) *Colour (pdf) |
F. Ellinghaus
prelim |
05-098 DVCS |
First cosine moment (fit method) of BCA on hydrogen and on deuterium as function of t-constraint compared to VGG model with different ansatzes for the parametrisations Aug 10, 2004 *Colour (eps) *Colour (pdf) INFO: This plot corresponds to the data shown in 06-020 (p) and 04-043. |
F. Ellinghaus
prelim |
02-089 DVCS |
t-distribution of the photon yields for H, D, Ne 2000 Data Sep 4, 2002 *Colour (eps) *Colour (pdf) |
F. Ellinghaus and J. Volmer
prelim |
02-088 DVCS nuclear |
beam-spin sin_{phi}-Moment from neon 2000 Data Sep 4, 2002 *Colour (eps) *Colour (pdf) |
F. Ellinghaus and J. Volmer
prelim |
02-087 DVCS deuterium |
beam-spin sin_{phi}-Moment from deuteron 2000 Data Sep 4, 2002 *Colour (eps) *Colour (pdf) |
F. Ellinghaus and J. Volmer
prelim |
02-086 DVCS proton |
beam-spin sin_{phi}-Moment from hydrogen 2000 Data Sep 4, 2002 *Colour (eps) *Colour (pdf) |
F. Ellinghaus and J. Volmer
prelim |
02-085 DVCS nuclear |
beam-spin asymmetry from neon 2000 Data Sep 4, 2002 *Colour (eps) *Colour (pdf) |
F. Ellinghaus and J. Volmer
prelim |
02-084 DVCS deuterium |
beam-spin asymmetry from deuteron 2000 Data Sep 4, 2002 *Colour (eps) *Colour (pdf) |
F. Ellinghaus and J. Volmer
prelim |
02-083 DVCS proton |
beam-spin asymmetry from hydrogen 2000 Data Sep 4, 2002 *Colour (eps) *Colour (pdf) |
F. Ellinghaus and J. Volmer
prelim |
06-009 TRANSVERSE |
The asymmetry A(phi,phi_{S}) as function of phi and phi_{S} for pi^{+} 2006 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) INFO: supportive plot |
U. Elschenbroich
final |
05-106 DIAGRAM |
Diagram of polarized semi-inclusive DIS for a transverse polarized target, transversity case Jul 24, 2005 *Colour (eps) *Colour (pdf) *Colour (fig) |
U. Elschenbroich
final |
05-105 DIAGRAM |
Diagram of polarized semi-inclusive DIS for a transverse polarized target, sivers case Jul 24, 2005 *Colour (eps) *Colour (pdf) *Colour (fig) |
U. Elschenbroich
final |
05-081 TRANSVERSE |
The definitions of the azimuthal angle $\phi$ of the hadron production plane, relative to the plane containing the momentum $\vec{l}$ ($\vec{l}'$) of the incident (scattered) lepton May 16, 2005 *BW (eps) *BW (pdf) |
U. Elschenbroich
final |
05-080 TRANSVERSE |
The various azimuthal moments appearing in the measurement of the $\sin\phi$ modulations of single-spin asymmetries on a longitudinally polarised target. Open symbols: measured epton axis moments; the ones from a transversely polarised target are multiplied by $-\sin\theta_{gamma ^*}$. Closed symbols: subleading-twist contribution to the measured lepton-axis asymmetries on a longitudinally polarised target. An overall systematic error of 0.003 is not included in the figure May 16, 2005 *Colour *BW *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
U. Elschenbroich
final |
05-061 TRANSVERSE |
The definitions of the azimuthal angles of the hadron production plane and the axis of the relevant component $\vec{S}_\perp$ of the target spin, relative to the plane containing the momentum $\vec{k}$ ($\vec{k}'$) of the incident (scattered) lepton Mar 28, 2005 *BW (eps) *BW (pdf) |
U. Elschenbroich
final |
05-001 DIAGRAM |
Flashy diagram of DVCS-SSA-kinematics for a tranversely polarised target ('3d') Jan 30, 2005 *Colour *Colour (eps) *Colour (jpeg) *Colour (pdf) |
U. Elschenbroich
final |
04-001 DIAGRAM |
Flashy diagram of DVCS-SSA-kinematics ('3d') Jan 6, 2004 *Colour *Colour (eps) *Colour (jpeg) *Colour (pdf) |
U. Elschenbroich
final |
03-078 DIAGRAM |
a real transparent HERMES logo Sep 19, 2001 *Colour (eps) *Colour (pdf) *Colour (fig) |
U. Elschenbroich
final |
03-044 PR-PLOT |
The flags of all countries involved in HERMES May 10, 2003 *Colour (eps) *Colour (jpeg) *Colour (pdf) *Colour (fig) |
U. Elschenbroich
final |
03-004 AZIMUTHAL |
The table of results on SSA for exclusive rho production on deuteron Feb 5, 2003 *Colour *Colour (eps) *Colour (pdf) |
U. Elschenbroich
prelim |
03-003 AZIMUTHAL rho |
The sin\phi moment of SSA for exclusive rho versus x,Q^{2} and -t' compared to the results for exclusive electroproduction of pi^{+} Feb 5, 2003 *Colour *Colour (eps) *Colour (pdf) |
U. Elschenbroich
prelim |
03-002 AZIMUTHAL rho |
The sin\phi moment of SSA versus x,Q^{2} and -t' for exclusive rho production on deuteron Feb 5, 2003 *Colour *Colour (eps) *Colour (pdf) |
U. Elschenbroich
prelim |
03-001 AZIMUTHAL rho |
The phi-dependence of A_{UL} for exclusive rho on deuteron Feb 5, 2003 *Colour *Colour (eps) *Colour (pdf) |
U. Elschenbroich
prelim |
02-098 DIAGRAM |
Flashy diagram of SSA-kinematics for longitudinal target with all target spin directions('3d') Dec 2, 2002 *Colour *Colour (eps) *Colour (jpeg) *Colour (pdf) |
U. Elschenbroich
final |
02-097 DIAGRAM |
Flashy diagram of SSA-kinematics for longitudinal target('3d') Dec 2, 2002 *Colour *Colour (eps) *Colour (jpeg) *Colour (pdf) |
U. Elschenbroich
final |
02-096 DIAGRAM |
Flashy diagram of SSA-kinematics for transverse target('3d') Dec 2, 2002 *Colour *Colour (eps) *Colour (jpeg) *Colour (pdf) |
U. Elschenbroich
final |
01-106 DIAGRAM |
Flashy diagram of nucleon spin ('3d') Sep 19, 2001 *Colour (jpeg) |
U. Elschenbroich
final |
01-106a DIAGRAM |
Flashy diagram of nucleon spin ('3d') assuming only valence quarks Sep 19, 2001 *Colour (jpeg) |
U. Elschenbroich
final |
01-106b DIAGRAM |
Flashy diagram of nucleon spin ('3d') with angular momentum Sep 19, 2001 *Colour (jpeg) |
U. Elschenbroich
final |
01-105 DIAGRAM |
Flashy diagram of inclusive DIS scattering Sep 19, 2001 *Colour (jpeg) |
U. Elschenbroich
final |
01-105a DIAGRAM |
Flashy diagram of inclusive DIS scattering with quark and nucleon spin anti-aligned Sep 19, 2001 *Colour (jpeg) |
U. Elschenbroich
final |
01-105b DIAGRAM |
Flashy diagram of inclusive DIS scattering with quark and nucleon spin aligned Sep 19, 2001 *Colour (jpeg) |
U. Elschenbroich
final |
02-016 DVCS proton |
The beam-spin analyzing power A_{LU}^{sin} phi for hard electroproduction of photons on hydrogen 96/97 data as a function of x Bjorken. The systematic uncertainty is represented by the error band at the bottom of the figure Feb 26, 2002 *Colour (eps) *Colour (pdf) |
J. Ely
prelim |
02-015 DVCS proton |
The beam-spin analyzing power A_{LU}^{sin} phi for hard electroproduction of photons on hydrogen 96/97 data as a function of t. The systematic uncertainty is represented by the error band at the bottom of the figure Feb 26, 2002 *Colour (eps) *Colour (pdf) |
J. Ely
prelim |
02-014 DVCS proton |
The beam-spin analyzing power A_{LU}^{sin} phi for hard electroproduction of photons on hydrogen 96/97 data as a function of Q^{2}. The systematic uncertainty is represented by the error band at the bottom of the figure Feb 26, 2002 *Colour (eps) *Colour (pdf) |
J. Ely
prelim |
01-076 DVCS proton |
The beam-spin analyzing power A_{LU}^{sin} phi for hard electroproduction of photons on hydrogen as a function of the missing mass. The systematic uncertainty is represented by the error band at the bottom of the figure Jun 27, 2001 *Colour (eps) *Colour (pdf) *Data |
J. Ely
final |
01-075 DVCS proton |
The sin phi-moment A_{LU}^{sin} phi^+/- as a function of the missing mass for positive beam helicity (circles), negative beam helicity (squares) and the averaged helicity (open triangles). A negative value is assigned to M_{x} if M_{x}^{2} lt 0. The error bars are statistical only. The systematic uncertainty is represented by the error band at the bottom of the figure Jun 27, 2001 *Colour (eps) *Colour (pdf) *Data |
J. Ely
final |
01-074 DVCS proton |
Beam-spin asymmetry A_{LU} for hard electroproduction of photons as a function of the azimuthal angle phi. The data correspond to the missing mass region between -1.5 and +1.7 GeV. The dashed curve represents a sin phi dependence with an amplitude of 0.23, while the solid curve represents the result of an SPD calculation taken from Ref.16. The horizontal error bars represent the bin width, and the error band below represents the systematic uncertainty Jun 27, 2001 *Colour (eps) *Colour (pdf) *Data |
J. Ely
final |
01-073 DVCS proton |
The measured distribution of photons observed in hard electroproduction versus the missing mass squared M_{x}^{2}. In the upper panel the full kinematic range is displayed, while the low M_{x}^{2} domain is shown in the lower panel. The light-gray histogram represents the results of a Monte-Carlo simulation in which fragmentation processes and the Bethe-Heitler process are included, while the dark-shaded histogram represents only the BH contribution. The Monte-Carlo simulation includes the effect of the detector resolution Jun 27, 2001 *Colour (eps) *Colour (pdf) |
J. Ely
final |
01-072 DVCS proton |
(a) Feynman diagram for deeply-virtual Compton scattering, and (b) photon radiation from the incident and scattered lepton in the Bethe-Heitler process Jun 27, 2001 *Colour (eps) *Colour (pdf) |
J. Ely
final |
00-035 DVCS proton |
The distribution of events as a function of missing mass squared Sep 1, 2000 *Colour *Colour (eps) *Colour (pdf) |
J. Ely
prelim |
Author: F | ||
Back to top | ||
04-076a EXCLUSIVE 2pion |
for explanation see 04-076b Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-076b EXCLUSIVE 2pion |
The x-dependence of the Legendre moments< P_{1} > for both targets separately, in the regions 0.30 |
R. fabbri
final |
04-075a EXCLUSIVE 2pion |
for explanation see 04-075d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-075b EXCLUSIVE 2pion |
for explanation see 04-075d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-075c EXCLUSIVE 2pion |
for explanation see 04-075d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-075d EXCLUSIVE 2pion |
The m_{\pi\pi}-dependence} of \la P_{1} + 7/3 \cdot P_{3} \ra (04-075a/b) and \la P_{1} - 14/9 \cdot P_{3} \ra (04-075c/d) for hydrogen (04-075a/c) and deuterium (04-075b/d). The data have \la x \ra =0.16, \la Q^{2} \ra = 3.2 (3.3) GeV^{2}}, and \la -t \ra = 0.43 (0.29) GeV^{2} for hydrogen (deuterium). The systematic uncertainty is represented by the error band Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-074a EXCLUSIVE 2pion |
for explanation see 04-074d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
R. fabbri
final |
04-074b EXCLUSIVE 2pion |
for explanation see 04-074d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-074c EXCLUSIVE 2pion |
for explanation see 04-074d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-074d EXCLUSIVE 2pion |
The m_{\pi\pi}-dependence of the Legendre moments \la P_{1} \ra (04-074a/b) and \la P_{3} \ra (04-074c/d) for hydrogen (04-074a/c) and deuterium (04-074b/d), for x>0.1. The region 0.8 Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-073a EXCLUSIVE 2pion |
Invariant mass spectrum for hydrogen for \Delta E<0.625 GeV (solid points) and \Delta E<0.125 GeV} (shaded area). For the spectrum the requirement x>0.1 has been applied. The m_{\pi\pi}-spectrum} for \Delta E<0.125 GeV is normalized and superimposed (shaded area) to show the suppression of the \omega ---> \pi^+\pi^-\pi^{0} contamination Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-073b EXCLUSIVE 2pion |
Invariant mass spectrum for deuterium for \Delta E<0.625 GeV (solid points) and \Delta E<0.125 GeV} (shaded area). For the spectrum the requirement x>0.1 has been applied. The m_{\pi\pi}-spectrum} for \Delta E<0.125 GeV is normalized and superimposed (shaded area) to show the suppression of the \omega ---> \pi^+\pi^-\pi^{0} contamination Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-072a EXCLUSIVE 2pion |
Distribution of pi^+pi^- events versus $\Delta E$ for hydrogen with 0.60 < m_{pipi} < 0.95 GeV}. The data are represented by the solid circles, while the simulated (SIDIS) background is represented by the histogram. The Monte Carlo results are normalized to the data using the region of the spectrum above \Delta E>2 GeV Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-072b EXCLUSIVE 2pion |
Yield of the exclusive events as obtained by subtracting the normalized Monte Carlo events from the data. The result (thin line) of an arbitrarily normalized Monte Carlo simulation using the diffractive \rho^{0} DIPSI generator is superimposed on the exclusive distribution Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-071a EXCLUSIVE 2pion |
for explanation see 04-071d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-071b EXCLUSIVE 2pion |
for explanation see 04-071d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-071c EXCLUSIVE 2pion |
for explanation see 04-071d Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
04-071d EXCLUSIVE 2pion |
Leading twist diagrams for the hard exclusive reaction e^+ T ---> e^+ T' pi^+ pi^-$. Gluon exchange (a) gives rise to pions in the isovector state only, while the quark exchange mechanism (b,c,d) gives rise to pions in both isoscalar and isovector states Oct 18, 2004 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
R. fabbri
final |
03-048 G1 duality |
A_{1} vs x for both the resonance and DIS regions, demonstrating that quark-hadron duality holds in the spin sector May 20, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
A. Fantoni
final |
98-080 G1 gdh |
Cross section difference for the neutron from the GDH analysis 1998 *Colour *Colour (eps) *Colour (pdf) |
A. Fantoni
final |
98-079 G1 gdh |
Cross section difference for the proton from the GDH analysis 1998 *Colour *Colour (eps) *Colour (pdf) |
A. Fantoni
final |
98-078 G1 gdh |
DIS contribution to the GDH integral for the neutron 1998 *Colour *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
A. Fantoni
final |
98-077 G1 gdh |
DIS contribution to the GDH integral for the proton 1998 *Colour *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
A. Fantoni
final |
98-076 G1 gdh |
Cross section difference for proton and neutron from the GDH analysis 1998 *Colour *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
A. Fantoni
final |
98-075 G1 gdh |
Kinematic plane (Q^{2},nu) of the GDH analysis 1998 *BW *BW (eps) *BW (pdf) |
A. Fantoni
final |
96-100 FRAGMENTATION k0_s |
K 0 S Reconstruction 1996 *Colour (eps) *Colour (pdf) |
M.-A. Funk
prelim |
96-098 EXPERIMENT tracking |
Event display with labelled detectors, showing a 3-track event 1996 *Colour *Colour (eps) *Colour (pdf) |
M.-A. Funk
final |
Author: G | ||
Back to top | ||
11-082 F2 |
The world data on F^{d}_{2} as a function of Q^{2} in the kinematic region 0.0008 < x < 0.85 and 0.03 < Q^{2} < 300 GeV^{2}, overlapped with the phenomenological parameterization GD11-D Aug 1, 2011 *Colour (eps) *Colour (pdf) INFO: Supportive plot. |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-081 F2 |
The world data on F^{p}_{2} as a function of Q^{2} in the kinematic region 0.00006 < x < 0.85 and 0.03 < Q^{2} < 1000 GeV^{2}, overlapped with the phenomenological parameterization GD11-D Aug 1, 2011 *Colour (eps) *Colour (pdf) INFO: Supportive plot. |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-080 F2 |
Same as 11-073, HERMES data for F^{d}_{2} together with world data as a function of Q^{2}, but in the kinematic region where there is overlap with existing data Aug 1, 2011 *Colour (eps) *Colour (pdf) INFO: Supportive plot. |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-079 F2 |
Same as 11-072, HERMES data for F^{p}_{2} together with world data as a function of Q^{2}, but in the kinematic region where there is overlap with existing data Aug 1, 2011 *Colour (eps) *Colour (pdf) INFO: Supportive plot |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-078 F2 |
Same as 11-073, HERMES data for F^{d}_{2} together with world data as a function of Q^{2}, but in the kinematic region where there is only HERMES data Aug 1, 2011 *Colour (eps) *Colour (pdf) INFO: Supportive plot |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-077 F2 |
Same as 11-072, HERMES data for F^{p}_{2} together with world data as a function of Q^{2}, but in the kinematic region where there is only HERMES data Aug 1, 2011 *Colour (eps) *Colour (pdf) INFO: Supportive plot |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-076 F2 |
The Q^{2} dependence of sigma_{d}/sigma_{p} for data from SLAC, HERMES, EMC, NMC, JLAB and BCDMS in bins of x. The error bars on the data points represent total uncertainties. The data points are overlaid with the results from the fit described by the functional form A(x) + B(x) ln Q^{2} (blue solid line), with the unity line (red dashed) and with the ratio of the GD11-D over GD11-P fits (green dash-dotted line) Aug 1, 2011 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-075 F2 |
HERMES data for the photon-deuteron cross section as a function of W^{2}, together with world data and the results from the GD11-D fit (central curves) and its uncertainties (outer curves), in bins of Q^{2}. The data points denoted real photon are for photoproduction. Inner error bars are statistical uncertainties, while outer error bars are total uncertainties calculated as the sum in quadrature of all statistical and systematic uncertainties including normalization Aug 1, 2011 *Colour (eps) *Colour (pdf) |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-074 F2 |
HERMES data for the photon-proton cross section as a function of W^{2}, together with world data and the results from the GD11-P fit (central curves) and its uncertainties (outer curves), in bins of Q^{2}. The data points denoted real photon are for photoproduction. Inner error bars are statistical uncertainties, while outer error bars are total uncertainties calculated as the sum in quadrature of all statistical and systematic uncertainties including normalization Aug 1, 2011 *Colour (eps) *Colour (pdf) |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-073 F2 |
HERMES data for F^{d}_{2} together with world data in the kinematic range 0.008 < x < 0.679 and 0.02 GeV^{2} < Q^{2} < 20 GeV^{2}. The results are overlaid with the phenomenological parameterization GD11-D (black solid central curve) and its uncertainty (outer curves). A bin-centering correction is applied to the data in order to match the central values of the x bins. The values of F_{d}^{2} are scaled by powers of 1.6. Inner error bars are statistical uncertainties, while outer error bars are total uncertainties calculated as the sum in quadrature of all statistical and systematic uncertainties including normalization Aug 1, 2011 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-072 F2 |
HERMES data for F^{p}_{2} together with world data in the kinematic range 0.008 < x < 0.679 and 0.02 GeV^{2} < Q^{2} < 20 GeV^{2}. The results are overlaid with the phenomenological parameterization GD11-P (black solid central curve) and its uncertainty (outer curves). A bin-centering correction is applied to the data in order to match the central values of the x bins. The values of F_{p}^{2} are scaled by powers of 1.6. Inner error bars are statistical uncertainties, while outer error bars are total uncertainties calculated as the sum in quadrature of all statistical and systematic uncertainties including normalization Aug 1, 2011 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-071 F2 |
Inelastic deuteron differential DIS cross section multiplied by a factor Q^{4} for the purpose of illustration and scaled by powers of 1.6, in the kinematic range 0.008 < x < 0.639 and 0.2 GeV^{2} < Q^{2} < 20 GeV^{2}. The results are overlaid with the phenomenological parameterization GD11-D (central curves) and its uncertainty (outer curves). The error bars represent the total uncertainties calculated as the sum in quadrature of all statistical and systematic uncertainties including normalization, and are smaller than the symbols Aug 1, 2011 *Colour (eps) *Colour (pdf) |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-070 F2 |
Inelastic proton differential DIS cross section multiplied by a factor Q^{4} for the purpose of illustration and scaled by powers of 1.6, in the kinematic range 0.008 < x < 0.639 and 0.2 GeV^{2} < Q^{2} < 20 GeV^{2}. The results are overlaid with the phenomenological parameterization GD11-P (central curves) and its uncertainty (outer curves). The error bars represent the total uncertainties calculated as the sum in quadrature of all statistical and systematic uncertainties including normalization, and are smaller than the symbols Aug 1, 2011 *Colour (eps) *Colour (pdf) |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-069 F2 |
Percentage of charge-symmetric background, calculated from the ratio of the charge-symmetric events to the total events in each bin, for the 2000 deuterium data. The symbols refer to the Q^{2} binning shown in 11-066 Aug 1, 2011 *Colour (eps) *Colour (pdf) |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-068 F2 |
Lepton identification efficiency (top) and hadron contamination (bottom) in the year 2000. The symbols refer to the Q^{2} binning shown in 11-066 Aug 1, 2011 *Colour (eps) *Colour (pdf) |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-067 F2 |
Trigger efficiencies for data taken in the year 2000 shown separately for the top and bottom spectrometer halves. The error bars represent only statistical uncertainties. The symbols refer to the Q^{2} bins shown in 11-066 Aug 1, 2011 *Colour (eps) *Colour (pdf) |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
11-066 F2 |
Binning in (x,Q^{2}) used in the analysis and kinematic acceptance of events. The kinematic region covered is limited by the geometrical acceptance in theta and constraints on y and W^{2}. The symbols mark the locations of the average values of (x,Q^{2}) of each bin. The symbols A to F denote bins with increasing Q^{2} at given x Aug 1, 2011 *Colour (eps) *Colour (pdf) |
D. Gabbert, E. Aschenauer, L. De Nardo
final |
07-081 BEC |
Results for Goldhaber radius r_{G} obtained in e^+e^- experiments Mar 18, 2008 *Colour (eps) *Colour (pdf) INFO: Supportive plot |
G. Gapienko and V. Korotkov
prelim |
07-080 BEC |
Results for chaoticity parameter lambda obtained in e^+e^- experiments Mar 18, 2008 *Colour (eps) *Colour (pdf) INFO: Supportive plot |
G. Gapienko and V. Korotkov
prelim |
07-079 BEC |
Results for Goldhaber radius r_{G} obtained in lN interactions. The HERMES points are from hydrogen target Mar 18, 2008 *Colour (eps) *Colour (pdf) |
G. Gapienko and V. Korotkov
prelim |
07-078 BEC |
Results for chaoticity parameter lambda obtained in lN interactions. The HERMES points are from hydrogen target Mar 18, 2008 *Colour (eps) *Colour (pdf) |
G. Gapienko and V. Korotkov
prelim |
07-077 BEC |
W-dependence of the BEC parameter r_{G} from hydrogen target Mar 18, 2008 *Colour (eps) *Colour (pdf) |
G. Gapienko and V. Korotkov
prelim |
07-076 BEC |
W-dependence of the BEC parameter lambda from hydrogen target Mar 18, 2008 *Colour (eps) *Colour (pdf) |
G. Gapienko and V. Korotkov
prelim |
07-075 BEC |
A-dependence of the BEC parameters r_{G} from hydrogen target Mar 18, 2008 *Colour (eps) *Colour (pdf) |
G. Gapienko and V. Korotkov
prelim |
07-074 BEC |
A-dependence of the BEC paramenter lambda from hydrogen target Mar 18, 2008 *Colour (eps) *Colour (pdf) |
G. Gapienko and V. Korotkov
prelim |
07-073 BEC |
T-dependence of the correlation function with the method of event mixing (MEM) Mar 18, 2008 *Colour (eps) *Colour (pdf) |
G. Gapienko and V. Korotkov
prelim |
07-072 BEC |
T-dependence of the correlation funtion with the method of unlike-sign hadron pairs Mar 18, 2008 *Colour (eps) *Colour (pdf) |
G. Gapienko and V. Korotkov
prelim |
98-028 FRAGMENTATION pion |
Favoured and unfavoured fragmentation functions in comparison to EMC (acceptance corrected) 1998 *Colour *Colour (eps) *Colour (pdf) |
P. Geiger
prelim |
97-017 FRAGMENTATION pion |
ratio of unfavoured to favoured pion fragmentation functions D-/D+ vs z in comparison to EMC 1997 *Colour *BW *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
P. Geiger
prelim |
13-016 AZIMUTHAL |
Difference between the amplitudes of negative and positive unidentifed hadrons within the kinematic range 0.023 < x < 0.27, 0.3 < y < 0.85, 0.2 < z < 0.75 and 0.05 < P_{h}\perp < 1.0 GeV. Closed and open symbols are for amplitudes extracted from hydrogen and deuterium targets, respectively. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-015 AZIMUTHAL |
Difference between the amplitudes of negative and positive kaons within the kinematic range 0.042 < x < 0.27, 0.3 < y < 0.7, 0.2 < z < 0.6, 0.2 < P_{h}\perp < 0.7 GeV. Closed and open symbols are for amplitudes extracted from hydrogen and deuterium targets, respectively. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-014 AZIMUTHAL |
Difference between the amplitudes of negative and positive pions within the kinematic range 0.023 < x < 0.27, 0.3 < y < 0.85, 0.2 < z < 0.75 and 0.05 < P_{h}\perp < 1.0 GeV. Closed and open symbols are for amplitudes extracted from hydrogen and deuterium targets, respectively. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-013 AZIMUTHAL |
cos phi amplitudes from a deuterium target for positive (upper panels) and negative (lower panels) unidentifed hadrons (triangles), pions (squares) and kaons (circles), integrated over the kinematic range 0.042 < x < 0.27, 0.3 < y < 0.7, 0.2 < z < 0.6, 0.2 < P_{h}\perp < 0.7 GeV. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-012 AZIMUTHAL |
cos 2phi amplitudes from a deuterium target for positive (upper panels) and negative (lower panels) unidentifed hadrons (triangles), pions (squares) and kaons (circles), integrated over the kinematic range 0.042 < x < 0.27, 0.3 < y < 0.7, 0.2 < z < 0.6, 0.2 < P_{h}\perp < 0.7 GeV. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-009 AZIMUTHAL |
cos phi amplitudes for positive (upper panels) and negative (lower panels) unidentifed hadrons integrated over the kinematic range of 0.023 < x < 0.27, 0.3 < y < 0.85, 0.2 < z < 0.75 and 0.05 < P_{h}\perp < 1.0 GeV. Closed and open squares are for amplitudes extracted from hydrogen and deuterium targets, respectively. The inner bar represents the statistical uncertainty; the outer bar is the total uncertainty, evaluated as the sum in quadrature of statistical and systematic uncertainties. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-008 AZIMUTHAL |
cos 2phi amplitudes for positive (upper panels) and negative (lower panels) unidentifed hadrons integrated over the kinematic range of 0.023 < x < 0.27, 0.3 < y < 0.85, 0.2 < z < 0.75 and 0.05 < P_{h}\perp < 1.0 GeV. Closed and open squares are for amplitudes extracted from hydrogen and deuterium targets, respectively. The inner bar represents the statistical uncertainty; the outer bar is the total uncertainty, evaluated as the sum in quadrature of statistical and systematic uncertainties. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-007 AZIMUTHAL |
cos phi amplitudes for positive (upper panels) and negative (lower panels) kaons integrated over the kinematic range of 0.042 < x < 0.27, 0.3 < y < 0.7, 0.2 < z < 0.6, 0.2 < P_{h}\perp < 0.7 GeV. Closed and open squares are for amplitudes extracted from hydrogen and deuterium targets, respectively. The inner bar represents the statistical uncertainty; the outer bar is the total uncertainty, evaluated as the sum in quadrature of statistical and systematic uncertainties. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-006 AZIMUTHAL |
cos 2phi amplitudes for positive (upper panels) and negative (lower panels) kaons integrated over the kinematic range of 0.042 < x < 0.27, 0.3 < y < 0.7, 0.2 < z < 0.6, 0.2 < P_{h}\perp < 0.7 GeV. Closed and open squares are for amplitudes extracted from hydrogen and deuterium targets, respectively. The inner bar represents the statistical uncertainty; the outer bar is the total uncertainty, evaluated as the sum in quadrature of statistical and systematic uncertainties. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-005 AZIMUTHAL |
cos phi amplitudes for positive (upper panels) and negative (lower panels) pions integrated over the kinematic range of 0.023 < x < 0.27, 0.3 < y < 0.85, 0.2 < z < 0.75 and 0.05 < P_{h}\perp < 1.0 GeV. Closed and open squares are for amplitudes extracted from hydrogen and deuterium targets, respectively. The inner bar represents the statistical uncertainty; the outer bar is the total uncertainty, evaluated as the sum in quadrature of statistical and systematic uncertainties. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-004 AZIMUTHAL |
cos 2phi amplitudes for positive (upper panels) and negative (lower panels) pions integrated over the kinematic range of 0.023 < x < 0.27, 0.3 < y < 0.85, 0.2 < z < 0.75 and 0.05 < P_{h}\perp < 1.0 GeV. Closed and open squares are for amplitudes extracted from hydrogen and deuterium targets, respectively. The inner bar represents the statistical uncertainty; the outer bar is the total uncertainty, evaluated as the sum in quadrature of statistical and systematic uncertainties. Points have been slightly shifted horizontally for visibility Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here |
F. Giordano and R. Lamb
final |
13-003 AZIMUTHAL |
Average kinematics for the integration range 0.042 < x < 0.27, 0.3 < y < 0.7, 0.2 < z < 0.6, 0.2 < P_{h}\perp < 0.7 GeV, as extracted from a 4pi Monte Carlo Feb 19, 2013 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 13-002. |
F. Giordano and R. Lamb
final |
13-002 AZIMUTHAL |
Average kinematics for the integration range 0.023 < x < 0.27, 0.3 < y < 0.85, 0.2 < z < 0.75 and 0.05 < P_{h}\perp < 1.0 GeV, as extracted from a 4pi Monte Carlo (shown here for positive hadrons on hydrogen; other cases exhibit only minor deviations). The data in multi-dimensional bins (900 bins), as well as the covariance matrices can be found in here Feb 19, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
F. Giordano and R. Lamb
final |
13-001 AZIMUTHAL |
Depiction of the azimuthal angle phi Feb 19, 2013 *Colour (eps) *Colour (pdf) |
F. Giordano and R. Lamb
final |
13-071 TRANSVERSE 2kaon |
Sin(2phi-phi_{S}) |0,0> moment in the non-resonant mass region for K+K as a function of M_{KK}, x, y, z, P_{h\perp} Dec 13, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
13-070 TRANSVERSE 2kaon |
Twist-3 sinphi_{S} |0,0> moment in the non-resonant mass region for K+K as a function of M_{KK}, x, y, z, P_{h\perp} Dec 13, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
13-069 TRANSVERSE 2kaon |
Pretzelosity |0,0> moment in the non-resonant mass region for K+K as a function of M_{KK}, x, y, z, P_{h\perp} Dec 13, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
13-068 TRANSVERSE 2kaon |
Collins |0,0> moment in the non-resonant mass region for K+K as a function of M_{KK}, x, y, z, P_{h\perp} Dec 13, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
13-067 TRANSVERSE 2kaon |
Sivers |0,0> moment in the non-resonant mass region for K+K as a function of M_{KK}, x, y, z, P_{h\perp} Dec 13, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
13-066 TRANSVERSE 2kaon |
Partial waves of the Collins moment near the phi-mass peak Dec 13, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
13-065 TRANSVERSE 2kaon |
Partial waves of the Sivers moment near the phi-mass peak Dec 13, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
13-054 TRANSVERSE 2pion |
Collins |2,-2> and |2,2> moments as a function of M_{\pi\pi} for \pi^{+}\pi^{0}, \pi^{-}\pi^{0}, and \pi^{+}\pi^{-} pair dihadrons. Statistical uncertainties are indicated by the horizontal error bars, and the combined statistical and systematic uncertainties are indicated by the full error bars Apr 17, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
13-053 TRANSVERSE 2pion |
Collins |1,1> as a function of M_{\pi\pi}, x, y, and, z for \pi^{+}\pi^{0} and \pi^{-}\pi^{0} pair dihadrons. Statistical uncertainties are indicated by the horizontal error bars, and the combined statistical and systematic uncertainties are indicated by the full error bars Apr 17, 2013 *Colour (eps) *Colour (pdf) |
S. Gliske and L. Pappalardo
prelim |
07-059 EXCLUSIVE phi |
Delta E distribution Mar 13, 2008 *Colour (eps) *Colour (pdf) INFO: supportive plot |
S. Gliske
prelim |
07-058 EXCLUSIVE phi |
M_{KK} distribution Mar 13, 2008 *Colour (eps) *Colour (pdf) INFO: supportive plot |
S. Gliske
prelim |
07-057 EXCLUSIVE phi |
A_{UT} 2002-2005 with L-T separation Mar 13, 2008 *Colour (eps) *Colour (pdf) |
S. Gliske
prelim |
12-015 VECTOR-MESONS spin density matrix elements |
Spin density matrix elements of exclusive phi and rho^{0} meson productions on deuteron May 23, 2012 *Colour (eps) *Colour (pdf) |
M. Golembiovskaya, A. Rostomyan, D. Veretennikov, S. Yaschenko
prelim |
12-014 VECTOR-MESONS spin density matrix elements |
Spin density matrix elements of exclusive phi and rho^{0} meson productions on proton May 23, 2012 *Colour (eps) *Colour (pdf) |
M. Golembiovskaya, A. Rostomyan, D. Veretennikov, S. Yaschenko
prelim |
12-013 VECTOR-MESONS spin density matrix elements |
Scaled spin density matrix elements of exclusive phi and rho^{0} meson productions on proton and deuteron May 23, 2012 *Colour (eps) *Colour (pdf) |
M. Golembiovskaya, A. Rostomyan, D. Veretennikov, S. Yaschenko
prelim |
12-012 VECTOR-MESONS spin density matrix elements |
Scaled spin density matrix elements of exclusive phi meson production on proton and deuteron extracted from 1998-2007 date sets May 23, 2012 *Colour (eps) *Colour (pdf) |
M. Golembiovskaya, A. Rostomyan, D. Veretennikov, S. Yaschenko
prelim |
12-011 VECTOR-MESONS spin density matrix elements |
Spin density matrix elements of exclusive phi meson production on proton and deuteron extracted from 1998-2007 date sets May 23, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry |
M. Golembiovskaya, A. Rostomyan, D. Veretennikov, S. Yaschenko
prelim |
01-121 LAMBDA fragmentation |
Invariant mass peak of inclusively detected Lambda (Anti-Lambda) for polarized and unpolarized targets (1996-2000) Dec 4, 2001 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-052 FRAGMENTATION k0_s |
K^{0}_{s} kinematics (cos(gamma,Lambda),M_{x},p_{T}**2) in comparison to MC 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-051 FRAGMENTATION k0_s |
K^{0}_{s} kinematics (Q^{2},x,y,x_{F}) in comparison to MC 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-050 LAMBDA fragmentation |
Anti-Lambda kinematics (cos(gamma,Lambda),M_{x},p_{T}**2) in comparison to MC 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-049 LAMBDA fragmentation |
Anti-Lambda kinematics (Q^{2},x,y,x_{F}) in comparison to MC 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-048 LAMBDA fragmentation |
Lambda kinematics (cos(gamma,Lambda),M_{x},p_{T}**2) in comparison to MC 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-047 LAMBDA fragmentation |
Lambda kinematics (Q^{2},x,y,x_{F}) in comparison to MC 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-040 EXPERIMENT silicon upgrade, lambda |
Lambda x_{F} distribution for long and short tracks and events from the Lambda Wheels 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-039 LAMBDA fragmentation |
Lambda kinematics (cos(gamma,Lambda),M_{x},p_{T}**2,z) 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-038 LAMBDA fragmentation |
Lambda kinematics (Q^{2},x,y,x_{F}) 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
98-037 LAMBDA fragmentation |
Lambda and Antilambda Mass peaks (96+97 data) 1998 *Colour *Colour (eps) *Colour (pdf) |
O. Grebenyuk
prelim |
Author: H | ||
Back to top | ||
07-054 EXCLUSIVE pion |
Cross section for exclusive pi^{+} production by virtual photons as a function of Q^{2} for three x_{B} bins and integrated over t' Mar 12, 2008 *Colour (eps) *Colour (pdf) *Data |
C. Hadjidakis and D. Hasch
final |
07-053 EXCLUSIVE pion |
Differential cross section for exclusive pi^{+} production by virtual photons as a function of -t' for four Q^{2} bins Mar 12, 2008 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
C. Hadjidakis and D. Hasch
final |
07-052 EXCLUSIVE pion |
Distributions of exclusive pi^{+} events within the HERMES acceptance as a function of Q^{2}, x_{B}, -t' and phi for data compared with an exclusive Monte Carlo simulation based on a GPD parametrization (Vanderhaegen, Guichon, Guidal) Mar 12, 2008 *BW (eps) *BW (pdf) |
C. Hadjidakis and D. Hasch
final |
07-051 EXCLUSIVE pion |
Squared missing mass dependence of the normalized-yield difference N_{pi}+ - N_{pi}- for data and PHYTHIA Monte Carlo (upper panel) and squared missing mass dependence of the normalized-yield after background subtraction procedure Mar 12, 2008 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
C. Hadjidakis and D. Hasch
final |
07-050 EXCLUSIVE pion |
Leading-order (left panel) and soft-overlap (right panel) diagram for exclusive pi^{+} electroproduction amplitude Mar 12, 2008 *BW (eps) *BW (pdf) |
C. Hadjidakis and D. Hasch
final |
04-067 EXCLUSIVE |
Diagramm illustrating exclusive meson production Sep 23, 2004 *Colour (eps) *Colour (pdf) INFO: supporting plot |
C. Hadjidakis
final |
01-070 AZIMUTHAL pi-proton |
Cross section asymmetries vs. phi for pi^{0}, pi^{+}, pi^{-} all together on one plot with fit to a sine function Jul 29, 2001 *Colour (eps) *Colour (pdf) |
D. Hasch
final |
01-070a AZIMUTHAL pi-proton |
Cross section asymmetries vs. phi for pi^{+}, pi^{-}, pi^{0} all together on one plot with fit to a sine function Jul 29, 2001 *Colour (eps) *Colour (pdf) |
D. Hasch
final |
01-022 AZIMUTHAL pi-proton |
Analysing power in the sin phi moment for pi ^0 (circles) compared to previous results for pi^+ (triangles) and pi^- (squares) as a function of the pion fractional energy z, the Bjorken variable x and of the pion transverse momentum P_{T}. Error bars include the statistical uncertainties only. The filled and open bands at the bottom of the panels represent the systematic uncertainties for neutral and charged pions, respectively. The data for charged pion production are slightly shifted in z, x, and P_{T} for clarity. The shaded areas show a range of predictions of a model calculation applied to the case of pi^{0} electroproduction (see our paper) Jul 29, 2001 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
D. Hasch
final |
01-022a AZIMUTHAL pi-proton |
Analysing power in the sin phi moment for pi^{0} (circles), pi^+ (triangles) and pi^- (squares) as a function of z. Error bars include the statistical uncertainties only. The bands at the bottom of the panel represent the systematic uncertainties for neutral and charged pions. The data for charged pion production are slightly shifted for clarity Jul 29, 2001 *Colour (eps) *Colour (pdf) |
D. Hasch
final |
01-022b AZIMUTHAL pi-proton |
Analysing power in the sin phi moment for pi^{0} (circles), pi^+ (triangles) and pi^- (squares) as a function of x. Error bars include the statistical uncertainties only. The bands at the bottom of the panel represent the systematic uncertainties for neutral and charged pions. The data for charged pion production are slightly shifted for clarity Jul 29, 2001 *Colour (eps) *Colour (pdf) |
D. Hasch
final |
01-022c AZIMUTHAL pi-proton |
Analysing power in the sin phi moment for pi^{0} (circles), pi^+ (triangles) and pi^- (squares) as a function of pt. Error bars include the statistical uncertainties only. The bands at the bottom of the panel represent the systematic uncertainties for neutral and charged pions. The data for charged pion production are slightly shifted for clarity Jul 29, 2001 *Colour (eps) *Colour (pdf) |
D. Hasch
final |
01-022d AZIMUTHAL pi-proton |
Analysing power in the sin phi moment for pi^{0} (circles), pi^+ (triangles) and pi^- (squares) as a function of the pion fractional energy z, the Bjorken variable x and of the pion transverse momentum P_{T}. Error bars include the statistical uncertainties only. The filled and open bands at the bottom of the panels represent the systematic uncertainties for neutral and charged pions, respectively. The data for charged pion production are slightly shifted in z, x, and P_{T} for clarity Jul 29, 2001 *Colour (eps) *Colour (pdf) |
D. Hasch
final |
01-022e AZIMUTHAL pi-proton |
Analysing power in the sin phi moment for pi^+ (triangles) as a function of the pion fractional energy z, the Bjorken variable x and of the pion transverse momentum P_{T}. Error bars include the statistical uncertainties only. The open band at the bottom of the panels represent the systematic uncertainties. The curves show a range of predictions of a model calculation applied to the case of pi^+ electroproduction (see our paper) Jul 29, 2001 *Colour (eps) *Colour (pdf) |
D. Hasch
final |
01-022f AZIMUTHAL pi-proton |
Analysing power in the sin phi moment for pi^{0} (circles) as a function of the pion fractional energy z, the Bjorken variable x and of the pion transverse momentum P_{T}. Error bars include the statistical uncertainties only. The open band at the bottom of the panels represent the systematic uncertainties. The curves show a range of predictions of a model calculation applied to the case of pi^{0} electroproduction (see our paper) Jul 29, 2001 *Colour (eps) *Colour (pdf) |
D. Hasch
final |
98-046 G1 proton |
Final result for x * g_{1}^{p} from 97 data in comparison to SLAC-E143 (Q^{2}=2 GeV**2) and SMC (Q^{2}=10 GeV**2) 1998 *Colour *Colour (eps) *Colour (pdf) |
D. Hasch
final |
98-045 G1 proton |
Final result for g_{1}^{p} from 97 data in comparison to SLAC-E143 (Q^{2}=2 GeV**2) and SMC (Q^{2}=10 GeV**2) 1998 *Colour *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
D. Hasch
final |
98-044 G1 proton |
Final result for g_{1}/F_{1} from 97 data in comparison to SLAC-E143 and SMC 1998 *Colour *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
D. Hasch
final |
98-043 G1 proton |
Final result for g_{1}/F_{1} from 97 data 1998 *Colour *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
D. Hasch
final |
11-030 FRAGMENTATION |
The multiplicity target-difference ratio (H-D) for pions as a function of Q^{2} in 4 z-bins. Only the statistical uncertainty is shown May 5, 2011 *Colour (eps) *Colour (pdf) |
A. Hillenbrand and S. J. Joosten
prelim |
11-029 FRAGMENTATION |
The multiplicity target-difference ratio (H-D) for pions as a function of p_{T} in 4 z-bins. Only the statistical uncertainty is shown May 5, 2011 *Colour (eps) *Colour (pdf) |
A. Hillenbrand and S. J. Joosten
prelim |
05-079 FRAGMENTATION |
Charged pion multiplicities as function of Q^{2} for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is compared to parametrisations of charged pion fragmentation function from S. Kretzer 2005 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-066 FRAGMENTATION |
Multiplicities of pi^{+} as function of z obtained from 2000 unpolarised hydrogen data. Inner errorbars represent the statistical uncertainty and outer errorbars the quadratic sum of statistical and systematic uncertainties. The latter contains the uncertainty due to the correction for radiative and smearing effects. The systematic error from RICH unfolding is shown as a symmetric yellow band (for the VMD corrected data set only). The data is evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) INFO: The data has been corrected for RICH misidentifications, charge symmetric background and radiative and smearing effects. It is shown with and without correction for diffractive processes (closed and open points). The contribution of diffractive processes was estimated using a tuned PYTHIA6 simulation. |
A. Hillenbrand
prelim |
04-065 FRAGMENTATION |
Multiplicities of pi^{-} as function of z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) INFO: see plot 04-066 for pi+ |
A. Hillenbrand
prelim |
04-064 FRAGMENTATION |
Multiplicities of K^{+} as function of z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) INFO: see plot 04-066 for pi+ |
A. Hillenbrand
prelim |
04-063 FRAGMENTATION |
Multiplicities of K^{-} as function of z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) INFO: see plot 04-066 for pi+ |
A. Hillenbrand
prelim |
04-062 FRAGMENTATION |
Multiplicities of pi^{+} as function of z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=25 GeV^{2} and compared to the D_{u}^{pi^{+}} FF from EMC Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-061 FRAGMENTATION |
Multiplicities of pi^{-} as function of z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=25 GeV^{2} and compared to the D_{u}^{pi^{-}} FF from EMC Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-060 FRAGMENTATION |
Multiplicities of pi^{+} as function of Q^{2} for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-059 FRAGMENTATION |
Multiplicities of pi^{-} as function of Q^{2} for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-058 FRAGMENTATION |
Multiplicities of K^{+} as function of Q^{2} for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-057 FRAGMENTATION |
Multiplicities of K^{-} as function of Q^{2} for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-056 FRAGMENTATION |
Charged pion multiplicities as function of xbj for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The multiplicities are compared to old results published in Eur.Phys.J C21(2001) 599-606 ("Multiplicity of Charged and Neutral Pions...") All data evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) INFO: The differences in the slope can be attributed to a different method of acceptance correction used in the old analysis. |
A. Hillenbrand
prelim |
04-055 FRAGMENTATION |
Charged pion multiplicities as function of xbj for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is compared to charged hadron multiplicities from EMC. All data evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-054 FRAGMENTATION |
Multiplicities of pi^{+} as function of x for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-053 FRAGMENTATION |
Multiplicities of pi^{-} as function of x for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-052 FRAGMENTATION |
Multiplicities of K^{+} as function of x for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
04-051 FRAGMENTATION |
Multiplicities of K^{-} as function of x for four different bins in z obtained from 2000 unpolarised hydrogen data. Errorbars and band like in plot 04-066 for pi^{+}. The data is evolved to a common Q^{2}=2.5 GeV^{2} Sep 6, 2004 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
03-042 EXPERIMENT rich |
P-Matrix for one track per detector half from IRT Apr 22, 2003 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
03-036 FRAGMENTATION |
Multiplicity of pi^{+/-}, K^{+/-}, p and pbar vs momentum compared to the Lund Monte Carlo with different tuning parameters Apr 4, 2003 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
03-035 FRAGMENTATION |
Multiplicity of pi^{+/-}, K^{+/-}, p and pbar vs z compared to the Lund Monte Carlo with different tuning parameters Apr 4, 2003 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
03-034 FRAGMENTATION |
Multiplicity of pi^{+/-}, K^{+/-}, p and pbar vs p_{T} compared to the Lund Monte Carlo with different tuning parameters Apr 4, 2003 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
03-033 FRAGMENTATION |
Multiplicity of pi^{+/-}, K^{+/-}, p and pbar vs x_{F} compared to the Lund Monte Carlo with different tuning parameters Apr 4, 2003 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
03-032 FRAGMENTATION |
Multiplicity of pi^{+/-}, K^{+/-}, p and pbar vs rapidity compared to the Lund Monte Carlo with different tuning parameters Apr 4, 2003 *Colour (eps) *Colour (pdf) |
A. Hillenbrand
prelim |
09-091 EXCLUSIVE pion |
Model predictions for the sin(phi-phi_{S}) Fourier amplitude as a function of -t'. The curves represents predictions of GPDmodel calculations. The full circles show the values of A^{sin}(phi-phi_{S})_{UT,\ell} is taken from Fig. 1 (entry 09-090). The error bars (bands) represent the statistical (systematic) uncertainties Dec 21, 2009 *Colour *Colour (eps) *Colour (pdf) *Data INFO: The data values are attached to this entry. |
I. Hristova
final |
09-090 EXCLUSIVE pion |
The set of six Fourier amplitudes (A_{UT,\ell}) describing the sine modulations of the single-spin azimuthal asymmetry for unpolarized (U) beam and transverse (T) target polarization, in bins of -t', x_{B}, and Q^{2}. The error bars (bands) represent the statistical (systematic) uncertainties. The results receive an additional 8.2% scale uncertainty corresponding to the target polarization uncertainty Dec 21, 2009 *Colour *Colour (eps) *Colour (pdf) *Data INFO: The data values are attached to this entry. |
I. Hristova
final |
09-090b EXCLUSIVE pion |
Top panel: for the suqared missing mass dependence of the normalised yield N_{pi}^+ and N_{pi}^- for data (points) and Pythia Monte Carlo (histograms). Middle panel: the difference N_{pi}^+-N_{pi}^- of the distributions of the top panel (including Pythia MC). Bottom panel: as the middle panel, but with an MC histogram from the exclusive event generator normalised to data. The inner error bars represent the statistical uncertainty and the outer error bars represent the quadratic sum of statistical and systematic uncertainties Dec 21, 2009 *Colour *Colour (eps) *Colour (pdf) *Data INFO: Supporting plot that is not shown in the publication. The data values are attached to this entry. |
I. Hristova
final |
Author: I | ||
Back to top | ||
12-004 G1 g2 |
The spin-structure function xg2 of the proton as a function of x. HERMES data are shown together with data from the E155, E143, and SMC experiments. The total error bars for the HERMES, E155, and E143 experiments represent the quadratic sum of the statistical and systematic uncertainties. The statistical uncertainties are indicated by the inner error bars. The error bars for the SMC experiment represent the statistical uncertainties only. The solid curve corresponds to the Wandzura-Wilczek relation evaluated at the average Q^{2} values of HERMES at each value of x. For the HERMES data, the closed (open) symbols represent data with < Q^{2} > > 1 GeV^{2} ( < Q^{2} > < 1 GeV^{2}) Mar 19, 2012 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to the entry 12-003. The corresponding correlation matrix in 9 and 23 bins are contained in the file attached to this entry. |
A. Ivanilov, S. Korotkov
final |
12-003 G1 g2 |
The virtual-photon asymmetry A2 of the proton as a function of x. HERMES data are shown together with data from the E155, E143, and SMC experiments. The total error bars for the HERMES, E155, and E143 experiments represent the quadratic sum of the statistical and systematic uncertainties. The statistical uncertainties are indicated by the inner error bars. The error bars for the SMC experiment represent the statistical uncertainties only. The solid curve corresponds to the Wandzura-Wilczek relation evaluated at the average Q^{2} values of HERMES at each value of x. For the HERMES data, the closed (open) symbols represent data with < Q^{2} > > 1 GeV^{2} ( < Q^{2} > < 1 GeV^{2}) Mar 19, 2012 *Colour (eps) *Colour (pdf) *Data INFO: The data values in 9 and 23 bins are contained in the file attached to this entry. The corresponding correlation matrix in 9 and 23 bins are contained in the file attached to the entry 12-004 |
A. Ivanilov, S. Korotkov
final |
12-002 G1 g2 |
The spin-structure function xg2(x;Q^{2}) of the proton as a function of Q^{2} for selected values of x. Data from the experiments E155 and E143 are presented also. The error bars represent the quadratic sum of the statistical and systematic uncertainties. The solid curve is the result of the Wandzura-Wilczek relation Mar 19, 2012 *Colour (eps) *Colour (pdf) |
A. Ivanilov, S. Korotkov
final |
Author: J | ||
Back to top | ||
14-019 UNPOL-PDF sea-flavour |
The strange-parton distribution xS (x, Q^{2} ) from the measured HERMES multiplicity for charged kaons evolved to Q^{2} = 2.5 GeV^{2} assuming \int D_{S}^{K} (z, Q^{2})dz = 1.27. The solid curve is a two-parameter fit with S(x)=(\int D_{S}^{K} (z, Q^{2})dz)^-1 x^{-0.867\pm0.019} e^{-x/(0.0331\pm0.0014)} (1-x). The dashed, dot-dash, dotted curves are as given in Fig. 2. The broad band is the \pm 1 sigma zone of allowed values predicted by the neural network (NNPDF2.3) reference set [14]. The band at the bottom represents the propagated experimental systematic uncertainties. A scale uncertainty of approximately 10% coming from the precision of \int D_{S}^{K} (z, Q^{2})dz is not shown Jun 25, 2014 *Colour (eps) *Colour (pdf) *Data |
H. E. Jackson
final |
14-018 UNPOL-PDF sea-flavour |
The product, S(x,Q^{2})\int D_{S}^{K} (z, Q^{2})dz, of the strange-quark PDF and the integral of the fragmentation function for strange quarks (squares) obtained from the measured HERMES multiplicity for charged kaons at the average Q^{2} for each bin. The solid curve is a least-squares fit with the result f(x)=x^{-0.834\pm0.019} e^{-x/(0.0337\pm0.0014)} (1-x). The band represents propagated experimental systematic uncertainties. The open points and the dashed curve show the data and fit published previously in Ref. [7] Jun 25, 2014 *Colour (eps) *Colour (pdf) *Data |
H. E. Jackson
final |
14-016 UNPOL-PDF sea-flavour |
The strange-parton distribution xS(x,Q^{2}) from the measured HERMES multiplicity for charged kaons evolved to Q^{2} = 2.5 GeV^{2} using the compilation of fragmentation functions (FFs) from [9] (DSS). The solid curve is a three-parameter fit to the data, the dashed curve gives xS(x) from CTEQ6L, and the dot-dash curve is the sum of light anti-quarks from CTEQ6L. The dotted curve is from CTEQ 6.5 S-0, a PDF reference set [10] in which the shape of xS(x) has not been constrained. The band containing the experimental points represents the fully correlated systematic uncertainties arising from the imprecision of \int D_{Q}^{K} (z, Q^{2})dz Jun 25, 2014 *Colour (eps) *Colour (pdf) *Data |
H. E. Jackson
final |
14-015 UNPOL-PDF sea-flavour |
The multiplicity of charged kaons in semi-inclusive DIS from a deuterium target, as a function of Bjorken x. The continuous curve is calculated from the strange-quark contribution taken from the fit in Fig. 3, together with the non-strange contribution as extracted from the high-x multiplicity data (see text). The green dashed (magenta dash-dotted) curve shows separately the nonstrange- (strange-) quark contribution to the multiplicity for that fit. The blue-dotted curve is the LO prediction obtained with CTEQ6L PDFs and fragmentation functions from [9]. The values of the average Q^{2} for each x bin are shown in the lower panel. The band represents systematic uncertainties Jun 25, 2014 *Colour (eps) *Colour (pdf) *Data |
H. E. Jackson
final |
08-024 DELTA-Q delta-s |
Non strange and strange quark helicity distributions at Q_{0}^{2}=2.5 GeV^{2}, as a function of Bjorken x. The curves are the LO results from Leader et al. from their analysis of world data Apr 4, 2008 *Colour (eps) *Colour (pdf) *Data |
H. Jackson
final |
08-023 DELTA-Q delta-s |
Lepton-nucleon polarized cross section asymmetries for inclusive and seminclusive DIS by a deuteron target as a function of Bjorken x, for identified charged kaons Apr 4, 2008 *Colour (eps) *Colour (pdf) |
H. Jackson
final |
08-022 DELTA-Q delta-s |
The strange parton distribution from the measured HERMES multiplicity for charged kaons evolved at Q_{0}^{2}=2.5 GeV^{2} Apr 4, 2008 *Colour (eps) *Colour (pdf) *Data |
H. Jackson
final |
08-021 DELTA-Q delta-s |
The strange fragmentation function product obtained from the measured HERMES multiplicity for charged kaons at the average Q^{2} for each bin Apr 4, 2008 *Colour (eps) *Colour (pdf) |
H. Jackson
final |
08-020 DELTA-Q delta-s |
The multiplicity corrected to 4pi of charged kaons in seminclusive DIS from a deuterium target, as a function of Bjorken x. The average Q^{2} for each bin are shown in the lower panel Apr 4, 2008 *Colour (eps) *Colour (pdf) |
H. Jackson
final |
97-001 EXPERIMENT administration |
HERMES Institutes in 1997 1997 *Colour *Colour (eps) *Colour (pdf) |
H. Jackson
final |
06-086 HADRON-ATTENUATION pt broadening |
x dependence of <p_{t}^{2}>_{A} / <p_{t}^{2}>_{D} for charged hadron (combined) production from ^{3}He, ^{4}He, N, Ne, Kr, Xe May 30, 2007 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
06-085 HADRON-ATTENUATION pt broadening |
z dependence of <p_{t}^{2}>_{A} / <p_{t}^{2}>_{D} for charged hadron (combined) production from ^{3}He, ^{4}He, N, Ne, Kr, Xe May 30, 2007 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
06-084 HADRON-ATTENUATION pt broadening |
contour plots of 2-dimensional (nu,z) dependence of <p_{t}^{2}>_{A} / <p_{t}^{2}>_{D} for charged hadron (combined) production from N, Ne, Kr, Xe May 30, 2007 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
06-083 HADRON-ATTENUATION pt broadening |
A^{1/3} dependence of <p_{t}^{2}>_{A} / <p_{t}^{2}>_{D} for charged hadron (combined) production from ^{3}He, ^{4}He, N, Ne, Kr, Xe in eight hadron-momentum bins May 30, 2007 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
06-082 HADRON-ATTENUATION pt broadening |
p dependence of <p_{t}^{2}>_{A} / <p_{t}^{2}>_{D} for charged hadron (combined) production from ^{3}He, ^{4}He, N, Ne, Kr, Xe May 30, 2007 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
06-081 HADRON-ATTENUATION pt broadening |
p dependence of <p_{t}^{2}>_{A} / <p_{t}^{2}>_{D} for charged kaon (combined) production from ^{4}He, Ne, Kr, Xe May 30, 2007 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
06-080 HADRON-ATTENUATION pt broadening |
p dependence of <p_{t}^{2}>_{A} / <p_{t}^{2}>_{D} for charged pion (combined) production from ^{3}He, ^{4}He, N, Ne, Kr, Xe May 30, 2007 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
01-068 FRAGMENTATION pt |
Avg Pt(h-)/avg Pt(h+) vs z for different Mx cuts for hydrogen 96+97 data Jul 3, 2001 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
01-067 FRAGMENTATION pt |
Average Pt (h+ and h-) for hydrogen to deuterium for 96+97 data May 5, 2001 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
01-066 FRAGMENTATION pt |
Pt^{2} vs W^{2} of h+ and h- for 96+97 data with hydrogen compared to EMC data May 5, 2001 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
01-065 FRAGMENTATION pt |
Pt vs W^{2} of h+ and h- for 96+97 data with hydrogen. A Monte Carlo comparison is included May 5, 2001 *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-078 FRAGMENTATION pt |
avg Pt^{2} vs z on hydrogen (h+/h- comparison to EMC) Oct 18, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-077 FRAGMENTATION pt |
avg Pt vs z on hydrogen (comparison to world data for all charged hadrons) Oct 18, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-076 FRAGMENTATION pt |
avg Pt vs z on hydrogen and deuterium (comparison to world data for h+/-,K^{0}_{s}) Oct 18, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-075 FRAGMENTATION pt |
avg Pt vs z on hydrogen (h+/- to pi^{+}/- comparison) Oct 13, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-074 FRAGMENTATION pt |
avg Pt vs z on deuterium (h+/- to pi^{+}/- comparison) Oct 13, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-073 FRAGMENTATION pt |
avg Pt vs x on hydrogen (for h+/- and K^{0}_{s}) for z>0.6 Oct 13, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-072 FRAGMENTATION pt |
avg Pt vs x on deuterium (for h+/- and K^{0}_{s}) for z>0.6 Oct 13, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-071 FRAGMENTATION pt |
avg Pt vs z on hydrogen (for h+/- and K^{0}_{s}) Oct 13, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
00-070 FRAGMENTATION pt |
avg Pt vs z on deuterium (for h+/- and K^{0}_{s}) Oct 13, 2000 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
99-077 FRAGMENTATION k0_s |
Invariant mass spectrum of K^{0}_{s} Nov 24, 1999 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
99-076 FRAGMENTATION k0_s |
Decay length of K^{0}_{s} Nov 24, 1999 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
99-075 FRAGMENTATION k0_s |
Multiplicity for K^{0}_{s} production, overlaid with data from EMC and FNAL and with two theoretical models Nov 24, 1999 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
99-074 FRAGMENTATION k0_s |
Fragmentation function from u to K^{0}_{s}, overlaid with two theoretical models Nov 24, 1999 *Colour *Colour (eps) *Colour (pdf) |
A. Jgoun
prelim |
13-032 FRAGMENTATION |
Comparison of the vector-meson-corrected multiplicities measured on the deuteron for various hadrons with LO calculations using CTEQ6L parton distributions and three compilations of fragmentation functions. Also shown are the values obtained from the HERMES Lund Monte Carlo. The statistical error bars on the experimental points are too small to be visible May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-031 FRAGMENTATION |
Comparison of the vector-meson-corrected multiplicities measured on the proton for various hadrons with LO calculations using CTEQ6L parton distributions and three compilations of fragmentation functions. Also shown are the values obtained from the HERMES Lund Monte Carlo. The statistical error bars on the experimental points are too small to be visible May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-030 FRAGMENTATION |
Multiplicities of kaons for the proton and the deuteron as a function of Q^{2} in four z bins. Positive charge is on the left and negative charge is on the right of each panel. Uncertainties are as in Fig. 4 May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-029 FRAGMENTATION |
Multiplicities of pions for the proton and the deuteron as a function of Q^{2} in four z bins. Positive charge is on the left and negative charge is on the right of each panel. Uncertainties are as in Fig. 4 May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-028 FRAGMENTATION |
Multiplicities of kaons for the proton and the deuteron as a function of xB in four z bins. Positive charge is on the left and negative charge is on the right of each panel. Uncertainties are as in Fig. 4 May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-027 FRAGMENTATION |
Multiplicities of pions for the proton and the deuteron as a function of xB in four z bins. Positive charge is on the left and negative charge is on the right of each panel. Uncertainties are as in Fig. 4 May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-026 FRAGMENTATION |
Multiplicities of kaons for the proton and the deuteron as a function of Ph\perp in four z bins. Positive charge is on the left and negative charge is on the right of each panel. Uncertainties are as in Fig. 4 May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-025 FRAGMENTATION |
Multiplicities of pions for the proton and the deuteron as a function of Ph\perp in four z bins. Positive charge is on the left and negative charge is on the right of each panel. Uncertainties are as in Fig. 4 May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-024 FRAGMENTATION |
The asymmetry A^{h}_{d-p} as a function of xB, for the pion multiplicities shown in Fig. 8. The statistical uncertainty is shown by the error bars, while the systematic uncertainty is given by the error bands May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include asymmetries at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-023 FRAGMENTATION |
The asymmetry A^{h}_{d-p} as a function of z, for the multiplicities shown in Fig. 4. The values given by a LO calculation using fragmentation functions from DSS and parton distributions from CTEQ6L are given by the solid curves May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include asymmmetries at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-022 FRAGMENTATION |
Ratios of measured Born multiplicities for a proton target with and without the correction for exclusive vector mesons as a function of z. The statistical error bars are too small to be visible May 8, 2013 *Colour (eps) *Colour (pdf) |
S. J. Joosten
final |
13-021 FRAGMENTATION |
Comparison of measured Born multiplicities for a proton target with and without the correction for exclusive vector mesons as a function of z. The open (closed) circles include (exclude) exclusive vector meson production. The statistical error bars are too small to be visible May 8, 2013 *Colour (eps) *Colour (pdf) *Data INFO: The data files also include multiplicities at low and high z values. The covariance matrices can be found here. |
S. J. Joosten
final |
13-020 FRAGMENTATION |
Multiplicities corrected for exclusive vector mesons as a function of z from a hydrogen target (full circles) and a deuterium target (empty squares). Error bars for the statistical uncertainties are too small to be visible. The systematic uncertainties are given by the error bands May 8, 2013 *Colour (eps) *Colour (pdf) INFO: The corresponding data files are attached in entries 13-031 and 13-032. |
S. J. Joosten
final |
13-019 FRAGMENTATION |
Fraction of mesons generated by the decay of exclusive vector mesons as a function of z, from PYTHIA. The widths of the bands indicate the uncertainty in the corresponding fractions. The vertical dashed lines are the limits in z used in the multiplicity extractions May 8, 2013 *Colour (eps) *Colour (pdf) |
S. J. Joosten
final |
13-018 FRAGMENTATION |
Born space in (x,Q^{2}) for the multiplicities extracted May 8, 2013 *Colour (eps) *Colour (pdf) |
S. J. Joosten
final |
13-017 FRAGMENTATION |
Schematic view of the HERMES spectrometer May 8, 2013 *Colour (eps) *Colour (pdf) |
S. J. Joosten
final |
Author: K | ||
Back to top | ||
99-081 G1 neutron |
x * g_{1}^{n} compared with E154 Jan 10, 2000 *BW (eps) *BW (pdf) |
R. Kaiser
final |
96-045 EXPERIMENT pid |
HERMES Particle Identification: PID3 vs TRD 1996 *Colour (eps) *Colour (pdf) |
R. Kaiser
final |
16-167 TRANSVERSE |
Three-dimensional positive-kaon cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-166 TRANSVERSE |
Three-dimensional positive-kaon cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-165 TRANSVERSE |
Three-dimensional positive-kaon cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-164 TRANSVERSE |
Three-dimensional positive-kaon cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-163 TRANSVERSE |
Three-dimensional positive-kaon cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-162 TRANSVERSE |
Three-dimensional positive-kaon cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-161 TRANSVERSE |
Three-dimensional positive-kaon cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-160 TRANSVERSE |
Three-dimensional positive-kaon cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-159 TRANSVERSE |
Three-dimensional positive-kaon cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-158 TRANSVERSE |
Three-dimensional positive-kaon worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-157 TRANSVERSE |
Three-dimensional positive-kaon worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-156 TRANSVERSE |
Three-dimensional positive-kaon worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-155 TRANSVERSE |
Three-dimensional positive-kaon sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-154 TRANSVERSE |
Three-dimensional positive-kaon sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-153 TRANSVERSE |
Three-dimensional positive-kaon sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-152 TRANSVERSE |
Three-dimensional positive-kaon sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-151 TRANSVERSE |
Three-dimensional positive-kaon sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-150 TRANSVERSE |
Three-dimensional positive-kaon sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-149 TRANSVERSE |
Three-dimensional positive-kaon pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-148 TRANSVERSE |
Three-dimensional positive-kaon pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-147 TRANSVERSE |
Three-dimensional positive-kaon pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-146 TRANSVERSE |
Three-dimensional positive-kaon sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-145 TRANSVERSE |
Three-dimensional positive-kaon sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-144 TRANSVERSE |
Three-dimensional positive-kaon sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-143 TRANSVERSE |
Three-dimensional positive-kaon Sivers lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-142 TRANSVERSE |
Three-dimensional positive-kaon Sivers lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-141 TRANSVERSE |
Three-dimensional positive-kaon Sivers lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-140 TRANSVERSE |
Three-dimensional positive-kaon Collins lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-139 TRANSVERSE |
Three-dimensional positive-kaon Collins lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-138 TRANSVERSE |
Three-dimensional positive-kaon Collins lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-137 TRANSVERSE |
Three-dimensional negative-kaon cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-136 TRANSVERSE |
Three-dimensional negative-kaon cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-135 TRANSVERSE |
Three-dimensional negative-kaon cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-134 TRANSVERSE |
Three-dimensional negative-kaon cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-133 TRANSVERSE |
Three-dimensional negative-kaon cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-132 TRANSVERSE |
Three-dimensional negative-kaon cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-131 TRANSVERSE |
Three-dimensional negative-kaon cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-130 TRANSVERSE |
Three-dimensional negative-kaon cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-129 TRANSVERSE |
Three-dimensional negative-kaon cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-128 TRANSVERSE |
Three-dimensional negative-kaon worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-127 TRANSVERSE |
Three-dimensional negative-kaon worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-126 TRANSVERSE |
Three-dimensional negative-kaon worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-125 TRANSVERSE |
Three-dimensional negative-kaon sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-124 TRANSVERSE |
Three-dimensional negative-kaon sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-123 TRANSVERSE |
Three-dimensional negative-kaon sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-122 TRANSVERSE |
Three-dimensional negative-kaon sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-121 TRANSVERSE |
Three-dimensional negative-kaon sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-120 TRANSVERSE |
Three-dimensional negative-kaon sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-119 TRANSVERSE |
Three-dimensional negative-kaon pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-118 TRANSVERSE |
Three-dimensional negative-kaon pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-117 TRANSVERSE |
Three-dimensional negative-kaon pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-116 TRANSVERSE |
Three-dimensional negative-kaon sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-115 TRANSVERSE |
Three-dimensional negative-kaon sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-114 TRANSVERSE |
Three-dimensional negative-kaon sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-113 TRANSVERSE |
Three-dimensional negative-kaon Sivers lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-112 TRANSVERSE |
Three-dimensional negative-kaon Sivers lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-111 TRANSVERSE |
Three-dimensional negative-kaon Sivers lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-110 TRANSVERSE |
Three-dimensional negative-kaon Collins lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-109 TRANSVERSE |
Three-dimensional negative-kaon Collins lepton-beam amplitude on a transversely polarized proton target as a function of z Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-108 TRANSVERSE |
Three-dimensional negative-kaon Collins lepton-beam amplitude on a transversely polarized proton target as a function of x Feb 18, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-100 TRANSVERSE |
Three-dimensional negative-pion cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-099 TRANSVERSE |
Three-dimensional negative-pion cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-098 TRANSVERSE |
Three-dimensional negative-pion cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-097 TRANSVERSE |
Three-dimensional negative-pion cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-096 TRANSVERSE |
Three-dimensional negative-pion cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-095 TRANSVERSE |
Three-dimensional negative-pion cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-094 TRANSVERSE |
Three-dimensional negative-pion cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-093 TRANSVERSE |
Three-dimensional negative-pion cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-092 TRANSVERSE |
Three-dimensional negative-pion cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-091 TRANSVERSE |
Three-dimensional negative-pion worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-090 TRANSVERSE |
Three-dimensional negative-pion worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-089 TRANSVERSE |
Three-dimensional negative-pion worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-088 TRANSVERSE |
Three-dimensional negative-pion sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-087 TRANSVERSE |
Three-dimensional negative-pion sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-086 TRANSVERSE |
Three-dimensional negative-pion sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-085 TRANSVERSE |
Three-dimensional negative-pion sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-084 TRANSVERSE |
Three-dimensional negative-pion sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-083 TRANSVERSE |
Three-dimensional negative-pion sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-082 TRANSVERSE |
Three-dimensional negative-pion sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-081 TRANSVERSE |
Three-dimensional negative-pion sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-080 TRANSVERSE |
Three-dimensional negative-pion sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-079 TRANSVERSE |
Three-dimensional negative-pion pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-078 TRANSVERSE |
Three-dimensional negative-pion pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-077 TRANSVERSE |
Three-dimensional negative-pion pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-076 TRANSVERSE |
Three-dimensional negative-pion Collins lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-075 TRANSVERSE |
Three-dimensional negative-pion Collins lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-074 TRANSVERSE |
Three-dimensional negative-pion Collins lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-073 TRANSVERSE |
Three-dimensional negative-pion Sivers lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-072 TRANSVERSE |
Three-dimensional negative-pion Sivers lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-071 TRANSVERSE |
Three-dimensional negative-pion Sivers lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-070 TRANSVERSE |
Three-dimensional positive-pion cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-069 TRANSVERSE |
Three-dimensional positive-pion cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-068 TRANSVERSE |
Three-dimensional positive-pion cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-067 TRANSVERSE |
Three-dimensional positive-pion cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-066 TRANSVERSE |
Three-dimensional positive-pion cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-065 TRANSVERSE |
Three-dimensional positive-pion cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-064 TRANSVERSE |
Three-dimensional positive-pion cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-063 TRANSVERSE |
Three-dimensional positive-pion cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-062 TRANSVERSE |
Three-dimensional positive-pion cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-061 TRANSVERSE |
Three-dimensional positive-pion worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-060 TRANSVERSE |
Three-dimensional positive-pion worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-059 TRANSVERSE |
Three-dimensional positive-pion worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-058 TRANSVERSE |
Three-dimensional positive-pion sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-057 TRANSVERSE |
Three-dimensional positive-pion sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-056 TRANSVERSE |
Three-dimensional positive-pion sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-055 TRANSVERSE |
Three-dimensional positive-pion sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-054 TRANSVERSE |
Three-dimensional positive-pion sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-053 TRANSVERSE |
Three-dimensional positive-pion sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-052 TRANSVERSE |
Three-dimensional positive-pion sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-051 TRANSVERSE |
Three-dimensional positive-pion sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-050 TRANSVERSE |
Three-dimensional positive-pion sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-049 TRANSVERSE |
Three-dimensional positive-pion pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-048 TRANSVERSE |
Three-dimensional positive-pion pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-047 TRANSVERSE |
Three-dimensional positive-pion pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-046 TRANSVERSE |
Three-dimensional positive-pion Collins lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-045 TRANSVERSE |
Three-dimensional positive-pion Collins lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-044 TRANSVERSE |
Three-dimensional positive-pion Collins lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-043 TRANSVERSE |
Three-dimensional positive-pion Sivers lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-042 TRANSVERSE |
Three-dimensional positive-pion Sivers lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-041 TRANSVERSE |
Three-dimensional positive-pion Sivers lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-040 TRANSVERSE |
Three-dimensional proton cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-039 TRANSVERSE |
Three-dimensional proton cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-038 TRANSVERSE |
Three-dimensional proton cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-037 TRANSVERSE |
Three-dimensional proton cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-036 TRANSVERSE |
Three-dimensional proton cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-035 TRANSVERSE |
Three-dimensional proton cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-034 TRANSVERSE |
Three-dimensional proton cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-033 TRANSVERSE |
Three-dimensional proton cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-032 TRANSVERSE |
Three-dimensional proton cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-031 TRANSVERSE |
Three-dimensional proton worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-030 TRANSVERSE |
Three-dimensional proton worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-029 TRANSVERSE |
Three-dimensional proton worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-028 TRANSVERSE |
Three-dimensional proton sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-027 TRANSVERSE |
Three-dimensional proton sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-026 TRANSVERSE |
Three-dimensional proton sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-025 TRANSVERSE |
Three-dimensional proton sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-024 TRANSVERSE |
Three-dimensional proton sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-023 TRANSVERSE |
Three-dimensional proton sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-022 TRANSVERSE |
Three-dimensional proton sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-021 TRANSVERSE |
Three-dimensional proton sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-020 TRANSVERSE |
Three-dimensional proton sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-019 TRANSVERSE |
Three-dimensional proton pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-018 TRANSVERSE |
Three-dimensional proton pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-017 TRANSVERSE |
Three-dimensional proton pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-016 TRANSVERSE |
Three-dimensional proton Collins lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-015 TRANSVERSE |
Three-dimensional proton Collins lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-014 TRANSVERSE |
Three-dimensional proton Collins lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-013 TRANSVERSE |
Three-dimensional proton Sivers lepton-beam amplitude on a transversely polarized proton target as a function of P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-012 TRANSVERSE |
Three-dimensional proton Sivers lepton-beam amplitude on a transversely polarized proton target as a function of z Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-011 TRANSVERSE |
Three-dimensional proton Sivers lepton-beam amplitude on a transversely polarized proton target as a function of x Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-010 TRANSVERSE |
One-dimensional proton and anti-proton cos(phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-009 TRANSVERSE |
One-dimensional proton and anti-proton cos(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-008 TRANSVERSE |
One-dimensional proton and anti-proton cos(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-007 TRANSVERSE |
One-dimensional proton and anti-proton worm-gear lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-006 TRANSVERSE |
One-dimensional proton and anti-proton sin(2phi+phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-005 TRANSVERSE |
One-dimensional proton and anti-proton sin(2phi-phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-004 TRANSVERSE |
One-dimensional proton and anti-proton sin(phiS) lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-003 TRANSVERSE |
One-dimensional proton and anti-proton pretzelosity lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-002 TRANSVERSE |
One-dimensional proton and anti-proton Collins lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
16-001 TRANSVERSE |
One-dimensional proton and anti-proton Sivers lepton-beam amplitude on a transversely polarized proton target as a function of x, z and P_{h}\perp Jan 20, 2016 *Colour (eps) *Colour (pdf) |
L. Pappalardo/G. Karyan
prelim |
05-091 DVCS proton |
The \phi dependence of the longitudinal target-spin asymmetry (LTSA) on hydrogen May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-090 DVCS deuterium |
The \phi dependence of the longitudinal target-spin asymmetry (LTSA) on deuterium May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-089 DVCS proton, deuterium |
The $\sin \phi$ moment (fit method) of longitudinal target-spin asymmetry (LTSA) on hydrogen and deuterium as function of t May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-088 DVCS proton, deuterium |
The $\sin 2\phi$ moment (fit method) of longitudinal target-spin asymmetry (LTSA) on hydrogen and deuterium as function of t May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-087 DVCS proton, deuterium |
The $\sin \phi$ moment (fit method) of longitudinal target-spin asymmetry (LTSA) on hydrogen and deuterium as function of t compared to VGG model predictions May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-086 DVCS proton, deuterium |
The $\sin 2\phi$ moment (fit method) of longitudinal target-spin asymmetry (LTSA) on hydrogen and deuterium as function of t compared to VGG model predictions May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-085 DVCS proton, deuterium |
The $\sin \phi$ moment (fit method) of longitudinal target-spin asymmetry (LTSA) on hydrogen and deuterium as function of x-Bjorken May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-084 DVCS proton, deuterium |
The $\sin 2\phi$ moment (fit method) of longitudinal target-spin asymmetry (LTSA) on hydrogen and deuterium as function of x-Bjorken May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-083 DVCS proton, deuterium |
The $\sin \phi$ moment (fit method) of longitudinal target-spin asymmetry (LTSA) on hydrogen and deuterium as function of Q^{2} May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
05-082 DVCS proton, deuterium |
The $\sin 2\phi$ moment (fit method) of longitudinal target-spin asymmetry (LTSA) on hydrogen and deuterium as function of Q^{2} May 26, 2005 *Colour (eps) *Colour (pdf) |
M. Kopytin
prelim |
16-107 BEC |
The parameters r_{G} (top panel) and Î» (bottom panel) are shown as a function of the target atomic mass A. The inner part of the error bars indicate the statistical uncertainty and the total error bars have systematic uncertainties added in quadrature. The horizontal lines correspond to the average value of the parameters Jan 31, 2016 *Colour (eps) *Colour (pdf) *Data |
V. Korotkov and G. Gapienko
final |
16-106 BEC |
Goldhaber radius r_{G}, as a function of W, obtained in lepton nucleon scattering experiments. Different markers are used to indicate the different methods for the construction of the reference sample and the kinds of uncertainties included Jan 31, 2016 *Colour (eps) *Colour (pdf) |
V. Korotkov and G. Gapienko
final |
16-105 BEC |
Parameter r_{G} (top panel) and Î» (bottom panel) as a function of W, obtained with MEM and MUS methods on hydrogen. The inner and outer error bars indicate the statistical and total uncertainties. For the latter the statistical and systematic uncertainties are added in quadrature Jan 31, 2016 *Colour (eps) *Colour (pdf) *Data |
V. Korotkov and G. Gapienko
final |
16-104 BEC |
Double ratio correlation function for like-sign hadron pairs obtained with MEM and MUS based on hydrogen target data Jan 31, 2016 *Colour (eps) *Colour (pdf) *Data |
V. Korotkov and G. Gapienko
final |
16-103 BEC |
Consistency check of the two chosen reference samples. The quantity R^{TST} is defined in the text. The curve is a linear fit to the data for T between 0.05 GeV and 1.3 GeV Jan 31, 2016 *Colour (eps) *Colour (pdf) |
V. Korotkov and G. Gapienko
final |
16-102 BEC |
Top panel: normalized experimental (stars) and simulated (line) distributions for unlike-sign hadron pairs as a function of the variable T. Bottom panel: the ratio of these experimental (exp) and simulated (MC) distributions Jan 31, 2016 *Colour (eps) *Colour (pdf) |
V. Korotkov and G. Gapienko
final |
16-101 BEC |
Schematic illustration of the Boseâ€“Einstein effect Jan 31, 2016 *Colour (eps) *Colour (pdf) |
V. Korotkov and G. Gapienko
final |
01-063 DVCS |
Predictions for statistical precision of DVCS at HERMES Run II (based on 2fb^-1) May 4, 2001 *Colour (eps) *Colour (pdf) |
V. Korotkov
prelim |
05-100 EXPERIMENT recoil |
Missing Mass spectrum showing the exclusive and the semi-inclusive area. The different backgrounds leaking into the exclusive region are explained. The left plot shows the misingmass without the using the information from the recoiling proton in the recoil detector the right one what happens using the recoil detector. The left plot is similiar to 05-099 or 05-099a Jul 24, 2005 *Colour (eps) *Colour (pdf) |
B. Krauss, R. Kaiser
prelim |
04-044 DVCS deuterium |
First cosine moment (fit method) of BCA on vector polarization balanced (i.e. vector polarization approx. 0, tensor polarization approx. 1) deuterium as function of t-constraint Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: As multi-dimensional binning is impossible due to statistics, an acceptance dependent discrepancy of up to 20% between the measured asymmetry-moment and the asymmetry-moment at the kinematic mean values of the bins can be expected. |
B. Krauss
prelim |
04-043 DVCS deuterium |
First cosine moment (fit method) of BCA on unpolarized deuterium as function of t-constraint Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: see above for uncertainty due to binning effect |
B. Krauss
prelim |
04-042 DVCS deuterium |
First cosine moment (fit method) of BCA on vector polarization balanced and on unpolarized deuterium as function of t-constraint Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: see above for uncertainty due to binning effect |
B. Krauss
prelim |
04-041 DVCS deuterium |
First cosine moment (fit method) of BCA on vector polarization balanced deuterium compared to BCA on unpolarized deuterium as function of t-constraint Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: see above for uncertainty due to binning effect |
B. Krauss
prelim |
04-040 DVCS deuterium |
BCA on vector polarization balanced (i.e. vector polarization approx. 0, tensor polarization approx. 1) deuterium as function of phi Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: supportive plot (not corrected for background) |
B. Krauss
prelim |
04-039 DVCS deuterium |
BCA on unpolarized deuterium as function of phi Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: supportive plot (not corrected for background) |
B. Krauss
prelim |
04-038 DVCS deuterium |
BCA on both, vector polarization balanced and unpolarized deuterium as function of phi Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: supportive plot (not corrected for background) |
B. Krauss
prelim |
04-037 DVCS deuterium |
First cosine moment (fit method) of BCA on vector polarization balanced deuterium (i.e vector polarization approx. 0, tensor polarization approx. 1) as function of Mx Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: supportive plot: shows that the asymmetry is only non-zero in the exclusive region |
B. Krauss
prelim |
04-036 DVCS deuterium |
First cosine moment (fit method) of BCA on unpolarized deuterium as function of Mx Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: supportive plot |
B. Krauss
prelim |
04-035 DVCS deuterium |
First cosine moment (fit method) of BCA on both, vector polarization balanced and unpolarized deuterium as function of Mx Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: supportive plot |
B. Krauss
prelim |
04-034 DVCS deuterium |
First cosine moment (fit method) of BCA on vector polarization balanced deuterium compared to BCA on unpolarized deuterium as function of Mx Aug 2, 2004 *Colour (eps) *Colour (pdf) INFO: supportive plot |
B. Krauss
prelim |
12-010 AZIMUTHAL |
Same as 12-009 in comparison with theoretical prediction Apr 26, 2012 *Colour (eps) *Colour (pdf) |
P. Kravchenko, L. De Nardo
prelim |
12-009 AZIMUTHAL |
Double longitudinal-spin asymmetry A_{LL}^{cos} (p_{h}\perp) for 0.023 < x < 0.1 (blue simbols) and 0.1 < x < 0.6 (red simbols) regions for proton (circles) and deuteron (squares) targets Apr 26, 2012 *Colour (eps) *Colour (pdf) |
P. Kravchenko, L. De Nardo
prelim |
12-008 AZIMUTHAL |
Same as 12-007 in comparison with theoretical prediction Apr 26, 2012 *Colour (eps) *Colour (pdf) |
P. Kravchenko, L. De Nardo
prelim |
12-007 AZIMUTHAL |
Double longitudinal-spin asymmetry A_{LL}^{cos} (z) for 0.023 < x < 0.1 (blue simbols) and 0.1 < x < 0.6 (red simbols) regions for proton (circles) and deuteron (squares) targets Apr 26, 2012 *Colour (eps) *Colour (pdf) |
P. Kravchenko, L. De Nardo
prelim |
12-006 AZIMUTHAL |
Same as 12-005 in comparison with theoretical prediction Apr 26, 2012 *Colour (eps) *Colour (pdf) |
P. Kravchenko, L. De Nardo
prelim |
12-005 AZIMUTHAL |
Double longitudinal-spin asymmetry A_{LL}^{cos} (x) for 0.2 < z < 0.4 (blue simbols) and 0.4 < z < 0.8 (red simbols) regions for proton (circles) and deuteron (squares) targets Apr 26, 2012 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry |
P. Kravchenko, L. De Nardo
prelim |
11-092 DELTA-Q |
Top: The derived polarized valence quark distribution x(Delta u_{v}(x) + Delta d_{v}(x)) from the pion-charge-difference asymmetry compared to that obtained from purity method. The four additional points (red open circles) at high x are obtained from g_{1}^{d} results. Bottom: The integral of Delta u_{v}(x) + Delta d_{v}(x) over the 0.023 < x < 0.9 range evaluated at Q^{2} = 2.5 GeV^{2} Oct 26, 2011 *Colour (eps) *Colour (pdf) |
P. Kravchenko, L. De Nardo
prelim |
11-091 DELTA-Q |
The derived polarized valence quark densities Delta u_{v}(x) and Delta d_{v}(x) from the pion-charge-difference asymmetry compared to those computed from purity method. The error bars show the statistical uncertainties. The systematic uncertainties are shown as bands Oct 26, 2011 *Colour (eps) *Colour (pdf) |
P. Kravchenko, L. De Nardo
prelim |
11-028 DELTA-Q |
The pion-charge-difference asymmetry A_{1} for the proton target, and he hadron-, pion-, kaon-charge-difference asymmetry for the deuteron target as a function of x. The error bars represent the statistical uncertainties, and the bands indicates the systematic uncertainty May 2, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
P. Kravchenko and J. Rubin
prelim |
11-027 DELTA-Q |
The semi-inclusive double-spin asymmetry A_{1} for charged pions on a longitudinally polarized hydrogen target and for charged pions and kaons on a longitudinally polarized deuterium target vs. z. The dependencies are shown for three different ranges in x-Bjorken (x). The error bars represent the statistical uncertainties, and the colored band indicates the systematic uncertainty May 2, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
P. Kravchenko and J. Rubin
prelim |
05-104 EXPERIMENT recoil |
^{3}D picture of the HERMES spectrometer with the recoil detector Jul 24, 2005 *Colour (jpeg) |
J. Kuhlmann, V. Prahl
final |
05-103 EXPERIMENT recoil |
^{3}D picture of the HERMES front region with the recoil detector Jul 24, 2005 *Colour (jpeg) |
J. Kuhlmann, V. Prahl
final |
05-102 EXPERIMENT spectrometer |
^{3}D picture of the HERMES front region with the polarised target Jul 24, 2005 *Colour (jpeg) |
J. Kuhlmann, V. Prahl
final |
05-101 EXPERIMENT spectrometer |
^{3}D picture of the HERMES spectrometer in different views Jul 24, 2005 *Colour (jpeg) |
J. Kuhlmann, V. Prahl
final |
05-101a EXPERIMENT spectrometer |
^{3}D picture of the HERMES spectrometer in different views Jul 24, 2005 *Colour (jpeg) |
J. Kuhlmann, V. Prahl
final |
05-101b EXPERIMENT spectrometer |
^{3}D picture of the HERMES spectrometer in different views Jul 24, 2005 *Colour (jpeg) |
J. Kuhlmann, V. Prahl
final |
05-101c EXPERIMENT spectrometer |
^{3}D picture of the HERMES spectrometer in different views Jul 24, 2005 *Colour (jpeg) |
J. Kuhlmann, V. Prahl
final |
05-101d EXPERIMENT spectrometer |
^{3}D picture of the HERMES spectrometer in different views Jul 24, 2005 *Colour (jpeg) |
J. Kuhlmann, V. Prahl
final |
05-101f EXPERIMENT spectrometer |
^{3}D picture of the HERMES spectrometer in different views Jul 24, 2005 *Colour (pdf) |
J. Kuhlmann, V. Prahl
final |
05-101g EXPERIMENT spectrometer |
^{3}D picture of the HERMES spectrometer in different views Jul 24, 2005 *Colour (pdf) |
J. Kuhlmann, V. Prahl
final |
Author: L | ||
Back to top | ||
10-057 HADRON-ATTENUATION |
Illustration of hadronization in a nuclear environment 2010 *Colour (eps) *Colour (pdf) |
I. Lehmann
final |
05-036 EXPERIMENT target |
The BRP measurements for the 2002/03 data taking period Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-035 EXPERIMENT target |
The TGA measurements for the 2002/03 data taking period Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-034 EXPERIMENT target |
A temperature scan with hydrogen taken in 1997 Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-033 EXPERIMENT target |
Measured atomic fraction as a function of the cell temperature for $T_{cell}<100\,$K for the deuterium running in 2000. No dependence on the temperature can be seen. The working temperature during normal operation was set to $T_{cell}=60\,$K Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-032 EXPERIMENT target |
Nuclear vector polarization $P_{z}^{BRP}$ as function of the cell temperature T measured in August 2000. No dependence on the temperature is observed. The operating temperature of the target during data collection was ^{60}K Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-031 EXPERIMENT target |
Vector/tensor polarization, $P^{BRP}$, measured by BRP during the year 2000 running period. Each symbol represents data averaged over a 72-hour bin. The tensor polarization (lower plot) was employed from July on Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-030 EXPERIMENT target |
Atomic fraction, $\alpha^{TGA}$ measured by TGA during the year 2000 running period. Each symbol represents data averaged over a 72-hour bin. The absolute bin averaged values are always above 0.9 Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-029 EXPERIMENT target |
The TGA measurements for the entire 1997 data taking period. The vertical dashed lines indicate HERA beam loss events which affected the cell surface properties, and the solid line indicates the replacement of the target cell Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-028 EXPERIMENT target |
The TGA measurements for the entire 1997 data taking period. The vertical dashed lines indicate HERA beam loss events which affected the cell surface properties, and the solid line indicates the replacement of the target cell Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-027 EXPERIMENT target |
Simulated correlation between the values measured by the TGA or BRP detectors and their corresponding density-weighted average values in the storage cell. The three solid curves represent the three scenarios for the state of the cell surface: homogeneous cell (HC), homogeneous beam tube (HBT), and inhomogeneous beam tube (IBT). The left figure shows the range for recombination and the right picture shows the range for wall depolarization. Acceptable uncertainties of $\alpha_{r}$ and $\depol_{WD}$ (differences among the three horizontal dotted lines) can be achieved only with $\alpha_{r}^{TGA}$ and $\depol_{WD}^{BRP}$ close to unity (vertical dotted lines). The corresponding uncertainty grows rapidly with increasing recombination or depolarization Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-026 EXPERIMENT target |
Possible beam-induced nuclear depolarizing resonances in the HERMES target. The frequency difference between pairs of hyperfine states whose transitions lead to nuclear depolarization are plotted as a function of the holding field. The frequency values are normalized to $\nu_{HERA}=10.42\,$MHz. The symbols representing the resonance conditions are clearly distinguishable for the $\pi$ transitions, while they overlap with each other in the case of $\sigma$ and $\pi\ket{3}\leftrightarrow\ket{6}$ transitions, which are separated by a difference in the intensity of the holding field $\Delta B_{T}$ of only 0.37\,mT. The dashed lines represent the working fields of the transversely (left) and longitudinally (right) polarized targets Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-025 EXPERIMENT target |
Measured fractional hyperfine populations vs. magnetic field for hydrogen for the various injection modes. The measured values are given by symbols, while the lines show a fit using the solutions of equation 28 Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-024 EXPERIMENT target |
Schematic layout of the BRP. The rf-transition units extend from z = 600 to 810 mm. The beam blocker at the entrance to the first 6-pole magnet ensures 100% rejection of atoms with $m_{s}=-\frac{1}{2}$. The beam shutter is used to measure the hydrogen contribution coming from dissociative water ionization Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-023 EXPERIMENT target |
Time spectrum of atomic count rates in the TGA. The vertical lines indicate the binning used to define the chopper positions open, undefined and closed Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-022 EXPERIMENT target |
Schematic view of the BRP/TGA vacuum system Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-021 EXPERIMENT target |
A schematic diagram of the Target Gas Analyzer. The gas of atoms and molecules diffuses through the extension tube and is collimated by two baffles before entering the ionizing volume. The chopper is used for background subtraction Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-020 EXPERIMENT target |
Hyperfine energy levels of hydrogen (left) and deuterium (right) atoms as a function of the magnetic holding field (Breit-Rabi diagram) and corresponding labeling. The field values are scaled with the corresponding critical field and energy values with the corresponding hyperfine energy Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-019 EXPERIMENT target |
Schematic view (from downstream of the electron beam) of the HERMES ABS with dissociator and collimator for beam formation. Two sets of sextupole magnets are located along the beam axis as are the high-frequency transitions. The axis of the ABS is tilted by $30^\circ$ downwards with respect to the horizontal plane Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-018 EXPERIMENT target |
The storage cell and its support flange Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-017 EXPERIMENT target |
Transverse magnet field uniformity measured along the {\it{z}} axis at the nominal field strength B=297 mT. Deviations of \Delta B_{y}=0.15 mT (vert.) and \Delta B_{x}=0.60 mT (horiz.) have been measured within the cell volume Mar 28, 2005 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
05-016 EXPERIMENT target |
Field strength of the longitudinal target magnet measured along the HERA beam direction {\it{z}}, covering the full length of the storage cell. The line shows a polynomial fit to the measurement Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-015 EXPERIMENT target |
Longitudinal target chamber and superconducting magnet viewed from downstream with respect to the HERA beam direction (left), and from above (right) Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
05-014 EXPERIMENT target |
Schematic view of the HERMES longitudinally polarized target. From left to right: Atomic Beam Source (ABS), target chamber with cell and magnet, and diagnostic system composed by Target Gas Analyzer (TGA) and Breit-Rabi Polarimeter (BRP). The locations of the radio-frequency transition (RFT) units are indicated Mar 28, 2005 *BW (eps) *BW (pdf) |
P. Lenisa
final |
04-007 EXPERIMENT target |
Summary of the existing measurements of the nuclear polarization of recombined molecules. The newly obtained HERMES measurement at 260 K with a holding field of 330 mT is compared to the measurement by AmPS and IUCF obtained at room temperature and magnetic holding fields of 28 mT and 440 mT respectively Feb 7, 2004 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
04-006 EXPERIMENT target |
A schematic layout of the HERMES hydrogen target. From left to right: injection tube for atomic beam source (ABS), target chamber with cell and magnet, sample tube taking gas to target gas analyzer (TGA) and Breit-Rabi polarimeter (BRP) Feb 7, 2004 *Colour (eps) *Colour (pdf) |
P. Lenisa
final |
10-056 HIGH-PT |
Feynman diagrams for hard subprocesses: a) \ordera{0} DIS, b) \ordera{1} Photon-Gluon Fusion, and c) \ordera{1} QCD Compton scattering Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-055 HIGH-PT |
Measured asymmetry for the anti-tagged category of events for positive (left) and negative (right) inclusive hadrons from hydrogen (top) and deuterium (bottom) targets as a function of p_{T(beam)}. The uncertainties are statistical only. There is an overall normalization uncertainty of 5.2% (3.9%) for hydrogen (deuterium). The curves show the Monte Carlo asymmetries for three different fixed values assumed for the gluon polarization Aug 21, 2010 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
P. Liebing and E.C. Aschenauer
final |
10-054 HIGH-PT |
Measured asymmetry for the tagged category of events for positive (left) and negative (right) inclusive hadrons from hydrogen (top) and deuterium (bottom) targets as a function of p_{T(\gamma^*)}. The uncertainties are statistical only. There is an overall experimental normalization uncertainty of 5.2% (3.9%) for hydrogen (deuterium). The curves show the Monte Carlo asymmetries for three different fixed values assumed for the gluon polarization Aug 21, 2010 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 10-055. |
P. Liebing and E.C. Aschenauer
final |
10-053 HIGH-PT |
Measured asymmetry for hadron pairs produced from hydrogen (left) and deuterium (right) targets as a function of the minimum value of $\sum{p_{T(beam)}^2}$. The uncertainties are statistical only. There is an overall experimental normalization uncertainty of 5.2% (3.9%) for hydrogen (deuterium). The curves show the Monte Carlo asymmetries for three different values assumed for the gluon polarization Aug 21, 2010 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
P. Liebing and E.C. Aschenauer
final |
10-052 HIGH-PT |
Contributions to hard p interactions: (a) VMD, (b) direct, and (c) anomalous. Only the basic graphs are illustrated; additional partonic activity is allowed in all three processes. The presence of spectator jets has been indicated by dashed lines, while full lines show partons that (may) give rise to high-p_{t} jets. The gray ovals represent multiparton wave functions. Anomalous states are built up from a perturbatively given q \bar q fluctuation, while VMD fluctuations allow no simple perturbative representation Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-051 HIGH-PT |
Top panels: Measured cross section in the HERMES acceptance for tagged hadrons as a function of x_{B} (left), Q^{2} (middle), and z (right) for positive (full points) and negative hadrons (open points) using a deuterium target. The lines show the tuned Pythia 6.2 calculation. Bottom panels: The corresponding ratios of the Pythia calculation to the measured cross section Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-050 HIGH-PT |
Cross sections for inclusive pi^{0} production from resolved photon, QCDC, and PGF processes simulated using Pythia (solid lines) compared to the LO pQCD calculations (full points). Simulation and calculation are done in the collinear approach at Q^{2} < 0.01 GeV^{2}, 0.2 < y < 0.9. Green/Grey lines: subprocess cross sections after varying the renormalization and factorization scales by factors of 1/2and 2 in the simulation Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-049 HIGH-PT |
The simulated cross section for inclusive pi^{0} production from the PGF subprocess vs. p_{T(beam)}, \hat{p}_T^{2}, and x for Q^{2} < 0.01 GeV^{2}, 0.2 < y < 0.9. The simulations are done using the collinear approach ((green/gray) solid line), the collinear approach together with intrinsic k_{T} for the partons in nucleon and photon (dashed line), and with intrinsic k_{T} together with fragmentation transverse momenta (solid line) Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-048 HIGH-PT |
Left panels: The measured double-spin inclusive asymmetry A_\parallel (full points) and two MC asymmetries (solid and dashed lines) based on different assumptions for the low-p_{T} subprocess asymmetry (top) and the process fractions vs. x_{B} (bottom) for tagged events on a hydrogen target. Right panels: Double-spin asymmetry vs. p_{T(beam)} for anti-tagged hadron on a hydrogen (top) and deuterium (bottom) target Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-047 HIGH-PT |
The cross sections and subprocess contributions, in the HERMES acceptance as a function of p_{T(beam)} for the anti-tagged category of events and a deuterium target (left: positively charged hadrons, right: negatively charged hadrons). Top: The measured cross section and that generated by Pythia . Second row: The ratio of these two cross sections. Also shown is the effect of the k-factor. Third row: The subprocess fractions from Pythia. Bottom two rows: The asymmetries and the asymmetries weighted with the subprocess fractions for each subprocess and for the gluon PDFs Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-046 HIGH-PT |
The cross sections and subprocess contributions, in the HERMES acceptance, as a function of p_{T(\gamma^*)} for the tagged category of events and a deuterium target (left: positively charged hadrons, right: negatively charged hadrons). Top: The measured cross section and that generated by Pythia . Second row: The ratio of these two cross sections. Third row: The subprocess fractions from Pythia. Bottom two rows: The asymmetries and the asymmetries weighted with the subprocess fractions for each subprocess and for the gluon PDFs Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-045 HIGH-PT |
The cross sections and subprocess contributions, in the HERMES acceptance, as a function of the minimum value of \sum{p_{T(beam)}^2} for the production of inclusive hadron pairs on a deuterium target. Top: The measured cross section and that generated by \Pythia. Second row: The ratio of these two cross sections. Third row: The subprocess fractions from \Pythia. Bottom two rows: The asymmetries and the asymmetries weighted with the subprocess fractions for each subprocess and for the gluon PDFs Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-044 HIGH-PT |
The range of generated x for different values of p_{T(beam)} calculated by \Pythia for all signal processes, for the anti-tagged category of events and a deuterium target Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-043 HIGH-PT |
The correlation of the average hard scattering < \hat p_{T}^{2} > of all signal subprocesses as calculated by \Pythia with the hadron p_{T} for inclusive hadrons as calculated for the experimental data for the deuterium target. Left: tagged category; Center: anti-tagged category; Right: hadron pairs category. The dotted line goes along < \hat{p}_T^{2} > = p_{T}^{2}(h) (< \hat{p}_T^{2} > = \sum{p_{T}^{2}}/2) and the vertical dashed line shows the minimum p_{T} (\sum{p_{T}^{2}}) used for the analysis Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-042 HIGH-PT |
The value of \dggpfact\ determined in the anti-tagged category for protons (top) and deuterons (bottom) and positive (full points) and negative (open points) hadrons as a function of p_{T}. Also shown are the values for the tagged (squares) and pairs (triangle) category at their average respective p_{T}. The uncertainties shown are statistical only Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-041 HIGH-PT |
Measured asymmetries with statistical uncertainties in four p_{T} bins for the anti-tagged category and a deuterium target, compared to calculated asymmetries using the two functions Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-040 HIGH-PT |
Functional forms used with the values and statistical uncertainty bands from the fits. Light shaded area: the total x range spanned by the data; dark shaded area: the range in x where the preponderance of the data lies Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-039 HIGH-PT |
The light gray band shows the total uncertainty of deltaG / G (x) vs. x with the statistical and total systematic uncertainty added in quadrature. The point shown represents delta G/G (< x >) at < x >=0.22. The inner error bar represents the statistical uncertainty and the outer the total uncertainty obtained by adding statistical and total systematic uncertainty in quadrature Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
10-038 HIGH-PT |
The gluon polarization deltaG / G (< x >) from HERMES extracted with fct.~1 (< x > = 0.22, < \mu^{2} > = 1.35 GeV^{2}) compared to the ones from COMPASS (low Q^{2}: \mu^{2}=3 GeV^{2}, high Q^{2}: \mu^{2}=2.4 GeV^{2}, open charm: \mu^{2}=13 GeV^{2}) and SMC (\mu^{2}=3.6 GeV^{2}) including statistical uncertainties (inner error bars) and total uncertainties (outer error bars). The x region of the data is indicated by the horizontal bars. Fit function fct.~1 is shown over the full x range spanned by the HERMES data. Also shown are a sample of curves from NLO pQCD fits (DSSV, and BB-09) at \mu^{2}=1.5 GeV^{2}. For clarity only the central values are shown Aug 21, 2010 *Colour (eps) *Colour (pdf) |
P. Liebing and E.C. Aschenauer
final |
01-043 HIGH-PT inclusive |
Subprocess fractions for ep to hX from PYTHIA 6.1 Apr 24, 2001 *Colour *BW *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
P. Liebing
prelim |
01-042 HIGH-PT inclusive |
A-parallel vs Pt for inclusive h^+/- and pi^+/- production Apr 24, 2001 *Colour *BW *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
P. Liebing
prelim |
05-004 DELTA-Q |
Quark flavour purities for a neutron target. Comparing the latest and best fragmentation tune (2004c) with the tune used in the delta-q analysis (2004a) Jan 1, 2005 *Colour *Colour (eps) *Colour (pdf) |
L.A. Linden-Levy
final |
05-003 DELTA-Q |
Quark flavour purities for a proton target. Comparing the latest and best fragmentation tune (2004c) with the tune used in the delta-q analysis (2004a) and purities using the fragmentation functions by St. Kretzer Jan 1, 2005 *Colour *Colour (eps) *Colour (pdf) |
L.A. Linden-Levy
final |
03-070 VECTOR-MESONS asymmetry |
A_|| for exclusive rho^{0} production vs p_{t} and and the energy of the rho^{0} in quasi-real photoproduction. Targets: proton and deuteron May 20, 2003 *Colour (eps) *Colour (pdf) *Data |
K. Lipka
final |
03-069 VECTOR-MESONS asymmetry |
A_{1} for exclusive rho^{0} production vs Q^{2} overlaid with a theory prediction. Targets: proton and deuteron. Results for quasi-real photoproduction data are included May 20, 2003 *Colour (eps) *Colour (pdf) |
K. Lipka
final |
03-068 VECTOR-MESONS asymmetry |
A_{1} for exclusive rho^{0} production vs -t overlaid with a theory prediction. Targets: proton and deuteron May 20, 2003 *Colour (eps) *Colour (pdf) |
K. Lipka
final |
03-067 VECTOR-MESONS asymmetry |
A_{1} for exclusive rho^{0} production vs x overlaid with a theory prediction. Targets: proton and deuteron May 20, 2003 *Colour (eps) *Colour (pdf) |
K. Lipka
final |
03-066 VECTOR-MESONS asymmetry |
Exclusive phi invariant mass spectrum and delta E (missing energy) distribution, both with fits May 20, 2003 *Colour (eps) *Colour (pdf) |
K. Lipka
final |
03-065 VECTOR-MESONS asymmetry |
Delta E (missing energy) distribution for exclusive rho^{0} production with fits May 20, 2003 *Colour (eps) *Colour (pdf) |
K. Lipka
final |
03-064 VECTOR-MESONS asymmetry |
Exclusive rho^{0} invariant mass distribution with fits May 20, 2003 *Colour (eps) *Colour (pdf) |
K. Lipka
final |
13-064 TRANSVERSE inclusive |
A^{sin\psi}_{UT} amplitudes for charged pions and kaons for the `anti-tagged' category and the two DIS subsamples with 0.2 < z < 0.7 and z > 0.7, respectively. Also shown are the relative fractions of the two DIS subsamples with respect to the total inclusive sample of the corresponding hadron species after correction for trigger efficiency. Positive (negative) particles are denoted by filled (open) symbols. Inner error bars show the statistical uncertainties and the total error bars represent statistical and systematic uncertainties added in quadrature. Not shown is an additional 8.8% scale uncertainty due to the precision of the measurement of the target polarization Dec 8, 2013 *Colour (eps) *Colour (pdf) *Data |
A. Lopez, A. Martinez de la Ossa
final |
13-063 TRANSVERSE inclusive |
A^{sin\psi}_{UT} amplitudes for charged pions and kaons as a function of x_{F} for various slices in P_{T}. Symbol definitions and additional 8.8% scale uncertainty as in Fig. 2 Dec 8, 2013 *Colour (eps) *Colour (pdf) *Data |
A. Lopez, A. Martinez de la Ossa
final |
13-062 TRANSVERSE inclusive |
A^{sin\psi}_{UT} amplitudes for charged pions and kaons as a function of P_{T} for various slices in x_{F}. Symbol definitions and additional 8.8% scale uncertainty as in Fig. 2 Dec 8, 2013 *Colour (eps) *Colour (pdf) *Data |
A. Lopez, A. Martinez de la Ossa
final |
13-061 TRANSVERSE inclusive |
A^{sin\psi}_{UT} amplitudes for charged pions and kaons as a function of x_{F}. Positive (negative) particles are denoted by closed (open) symbols. When visible, the inner error bars show the statistical uncertainties, while the total ones represent the quadratic sum of statistical and systematic uncertainties. Not shown is an additional 8.8% scale uncertainty due to the precision of the measurement of the target polarization. The bottom subpanels show the x_{F} dependence of the average P_{T}. Data points for negative particles are slightly shifted horizontally for legibility Dec 8, 2013 *Colour (eps) *Colour (pdf) *Data |
A. Lopez, A. Martinez de la Ossa
final |
13-060 TRANSVERSE inclusive |
A^{sin\psi}_{UT} amplitudes for charged pions and kaons as a function of P_{T}. Positive (negative) particles are denoted by closed (open) symbols. When visible, the inner error bars show the statistical uncertainties, while the total ones represent the quadratic sum of statistical and systematic uncertainties. Not shown is an additional 8.8% scale uncertainty due to the precision of the measurement of the target polarization. The bottom subpanels show the P_{T} dependence of the average x_{F}. Data points for negative particles are slightly shifted horizontally for legibility Dec 8, 2013 *Colour (eps) *Colour (pdf) *Data |
A. Lopez, A. Martinez de la Ossa
final |
13-059 TRANSVERSE inclusive |
The definition of the azimuthal angle $\psi$ Dec 8, 2013 *Colour (eps) *Colour (pdf) |
A. Lopez, A. Martinez de la Ossa
final |
10-010 TRANSVERSE inclusive |
The sin phi_{S} amplitudes of the inclusive asymmetry A_{UT} in dependence of x_{B}, measured with an electron beam (top) and a positron beam (center). The open (closed) circles identify the data with Q^{2} < 1 GeV^{2} (Q^{2} > 1 GeV^{2}). The error bars show the statistical uncertainties, while the error boxes show the systematic uncertainties. The asymmetries integrated over x_{B} are shown on the left. Bottom panel: average Q^{2} vs. x_{B} from data (squares), and the fraction of elastic background events to the total event sample from a Monte Carlo simulation (triangles) Jan 26, 2010 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
A. Lopez, L. de Nardo, A. de la Ossa
final |
05-013 EXOTICS pentaquark |
Invariant mass distribution of the p\pi^-\pi^-\pi^+$(plus c.c.) system, subject to the constraints in event topology discussed in the text. The mixed-event background is represented by the gray shaded histogram, which is normalized to the background component of the fitted curve described in the text. The arrow shows the hypothetical \Xi^{0}_{3/2} mass. The excess near 1.77GeV has a statistical significance of only 1.8 \sigma Mar 28, 2005 *Colour (eps) *Colour (pdf) |
W. Lorenzon
final |
05-012 EXOTICS pentaquark |
Invariant mass distribution of the p pi^- pi^- pi^- system, subject to the constraints in event topology discussed in the text. The mixed-event background is represented by the gray shaded histogram, which is normalized to the background component of the fitted curve described in the text. The arrow shows the hypothetical \Xi^{--}_{3/2} mass Mar 28, 2005 *Colour (eps) *Colour (pdf) |
W. Lorenzon
final |
05-011 EXOTICS pentaquark |
Invariant mass distribution of the p pi^- system and charge conjugated (c.c.) mode Mar 28, 2005 *Colour (eps) *Colour (pdf) |
W. Lorenzon
final |
05-010 EXOTICS pentaquark |
Invariant mass distribution of the p pi^-pi^- system and charge conjugated (c.c.) mode Mar 28, 2005 *Colour (eps) *Colour (pdf) |
W. Lorenzon
final |
04-033 EXOTICS pentaquark |
histogram showing invariant mass resulting of gmc-dcay simulating a particle with mass 1540 decaying to Kshort + p taking all detector responses into account 2004 *Colour (eps) *Colour (pdf) |
W. Lorenzon
final |
04-032 EXOTICS pentaquark |
schematic plot show the decay topology and the placed cuts for the theta^+ 2004 *Colour (eps) *Colour (pdf) |
W. Lorenzon
final |
97-030 EXPERIMENT polarimeters |
comparison of risetime curve of transverse and longitudinal polarimeter 1997 *Colour (eps) *Colour (pdf) |
W. Lorenzon
final |
97-029 EXPERIMENT polarimeters |
risetime curve longitudinal polarimeter 1997 *Colour *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
W. Lorenzon
final |
Author: M | ||
Back to top | ||
10-030 DVCS proton |
Amplitudes of the target-spin asymmetry A_{UL} sensitive to a combination of the Interference and squared-DVCS terms, for positrons incident on longitudinally polarised protons, as projections in -t, x_{B}, and Q^{2}. The leftmost column shows the asymmetry values when the extraction is performed in a single bin across the entire kinematic range of the data set. The error bars (open red bands) show the statistical (systematic) uncertainties and the solid blue bands represent the predictions from the ``VGG Regge'' GPD model.. There is an additional 4.2% scale uncertainty due to the precision of the measurement of the target polarisation. The fractional contributions from resonance production estimated from an MC model are presented in the bottom panel Jul 16, 2010 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
D. Mahon and M. Murray
final |
10-029 DVCS proton |
Amplitudes of the double-spin asymmetry A_{LL} sensitive to the Interference, squared-DVCS and squared-BH terms in the scattering amplitude, for polarised positrons incident on longitudinally polarised protons, as projections in -t, x_{B}, and Q^{2}. The leftmost column shows the asymmetry values when the extraction is performed in a single bin across the entire kinematic range of the data set. The error bars (open red bands) show the statistical (systematic) uncertainties and the solid blue bands represent the theoretical predictions from the ``VGG Regge'' GPD model. There is an additional 5.3% scale uncertainty due to the precision of the measurement of the beam and target polarisations. The fractional contributions from resonance production estimated from an MC model are presented in the bottom panel Jul 16, 2010 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 10-030. |
D. Mahon and M. Murray
final |
09-067 DVCS proton |
The double-spin asymmetry (A_{LL}) amplitudes in DVCS from a longitudinally polarized hydrogen target. Shown are the cos0\phi, the cos\phi and the cos2\phi amplitudes in bins of t, xB, or Q^{2}. Also shown is the integrated value presenting the data in a single bin. The bottom row gives for each bin the fraction of the 'associated' process where the proton is excited to a resonant state. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands. Also shown are model calculations using the 'VGG' code (Regge type ansatz). Please note that the A_{UL} amplitudes (LTSA) will only be released by the publication of the paper Nov 2, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to this entry. |
D. Mahon and M. Murray
prelim |
09-066 DVCS proton |
The double-spin asymmetry (A_{LL}) cos0\phi amplitude in DVCS from a longitudinally polarized hydrogen target, in bins of t, xB, or Q^{2}. Also shown is the integrated value presenting the data in a single bin. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands. Also shown are model calculations using the 'VGG' code (Regge type ansatz). Please note that the A_{UL} amplitudes (LTSA) will only be released by the publication of the paper Nov 2, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-067. |
D. Mahon and M. Murray
prelim |
09-065 DVCS proton |
The double-spin asymmetry (A_{LL}) cos\phi amplitude in DVCS from a longitudinally polarized hydrogen target, in bins of t, xB, or Q^{2}. Also shown is the integrated value presenting the data in a single bin. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands. Also shown are model calculations using the 'VGG' code (Regge type ansatz). Please note that the A_{UL} amplitudes (LTSA) will only be released by the publication of the paper Nov 2, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-067. |
D. Mahon and M. Murray
prelim |
09-064 DVCS proton |
The double-spin asymmetry (A_{LL}) cos2\phi amplitude in DVCS from a longitudinally polarized hydrogen target, in bins of t, xB, or Q^{2}. Also shown is the integrated value presenting the data in a single bin. The statistical uncertainties are indicated by the error bars, the systematic uncertainies by the error bands. Also shown are model calculations using the 'VGG' code (Regge type ansatz). Please note that the A_{UL} amplitudes (LTSA) will only be released by the publication of the paper Nov 2, 2009 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 09-067. |
D. Mahon and M. Murray
prelim |
17-006 EXCLUSIVE rho |
Comparison of amplitude ratios to those calculated in the Goloskokov-Kroll model Jun 16, 2017 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
17-005 EXCLUSIVE rho |
Comparison of the SDMEs s^{\lambda_{V}\lambda_{V^{\prime}}_{\lambda_{\gamma}\lambda_{\gamma^{\prime}}} obtained from the amplitude method (red circles) and from the SDME method (blue squares). The SDMEs are extracted in the entire kinematic region. The points in the shaded area show SDMEs that can be obtained only if the beam is longitudinally polarized in addition to the transverse target polarization required for all SDMEs here Jun 16, 2017 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
17-004 EXCLUSIVE rho |
Comparison of the SDMEs n^{\lambda_{V}\lambda_{V^{\prime}}_{\lambda_{\gamma}\lambda_{\gamma^{\prime}}} obtained from the amplitude method (red circles) and from the SDME method (blue squares). The SDMEs are extracted in the entire kinematic region. The points in the shaded area show SDMEs that can be obtained only if the beam is longitudinally polarized in addition to the transverse target polarization required for all SDMEs here Jun 16, 2017 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
17-003 EXCLUSIVE rho |
Comparison of the SDMEs u^{\lambda_{V}\lambda_{V^{\prime}}_{\lambda_{\gamma}\lambda_{\gamma^{\prime}}} obtained from the amplitude method (red circles) and from the SDME method (blue triangles). The SDMEs are extracted in the entire kinematic region. The points in the shaded area show SDMEs that can be obtained only if the beam is longitudinally polarized Jun 16, 2017 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
17-002 EXCLUSIVE rho |
Helicity-amplitude ratios obtained from the 25-parameter fit characterized by = 1.93 GeV^{2}, <-t^{\prime}> = 0.132 GeV^{2} |
S. Manaenkov
final |
17-001 EXCLUSIVE rho |
Definition of angles in the process eN -> e\rho^{0}N->e\pi^{+}\pi^{-}N. Here, \PHI is the angle between the \rho^{0} production plane and the lepton scattering plane in the CM system of virtual photon and target nucleon. The variables \theta and \phi are respectively the polar and azimuthal angles of the decay \pi^{+} in the \rho^{0}-meson rest frame, with the z axis being anti-parallel to the outgoing nucleon momentum. The XZ and xz planes both the \gamma^{\star} and \rho^{0} three-momenta Jun 16, 2017 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-065 EXCLUSIVE rho |
The same as 10-100 but for Re(T_{01}/T_{00}) May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-064 EXCLUSIVE rho |
The kinematic dependences of Re(T_{11}/T_{00}) and for proton and deuteron data from HERMES and H1. Inner error bars show the statistical uncertainty and the outer ones indicate statistical and systematic uncertainties added in quadrature May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-063 EXCLUSIVE rho |
The same as 10-098 but for Im(T_{1-1}/T_{00}) / (-t') May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-062 EXCLUSIVE rho |
The Q^{2} dependence of Re(T_{1-1}/T_{00})/(-t') for proton and deuteron data. Points show amplitude ratios after averaging over $-t'$ bins. Inner error bars show the statistical uncertainty and the outer ones indicate statistical and systematic uncertainties added in quadrature. Central lines are calculated with the fitted values of parameters, while the dashed lines correspond to one standard deviation of the curve parameter May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-061 EXCLUSIVE rho |
The same as 10-096 but for Im(T_{10}/T_{00})/\sqrt{-t'} May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-060 EXCLUSIVE rho |
The Q^{2} dependence of Re(T_{10}/T_{00}) / \sqrt{-t'} for proton and deuteron data. Points show amplitude ratios after averaging over -t' bins. Inner error bars show the statistical uncertainty and the outer ones indicate statistical and systematic uncertainties added in quadrature. Central lines are calculated with the fitted values of parameters, while the dashed lines correspond to one standard deviation of the curve parameter May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-059 EXCLUSIVE rho |
The same as 10-094 but for Im(T_{01}/T_{00}) / \sqrt{-t'} May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-058 EXCLUSIVE rho |
The Q^{2} dependence of Re(T_{01}/T_{00}) / \sqrt{-t'} for proton and deuteron data. Points show amplitude ratios after averaging over -t' bins. Inner error bars show the statistical uncertainty and the outer bars show statistical and systematic uncertainties added in quadrature. Central lines are calculated with fitted values of parameters, while the dashed lines correspond to one standard deviation of the curve parameter May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-057 EXCLUSIVE rho |
The same as 10-092 but for Q * Im (T_{01}/T_{00} ) May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-056 EXCLUSIVE rho |
The t' dependence of Re(T_{01}/T_{00}) for proton and deuteron data. Points show amplitude ratios after averaging over $Q^{2}$ bins. Inner error bars show the statistical uncertainty and the outer bars show statistical and systematic uncertainties added in quadrature. Central lines are calculated with fitted values of parameters, while the dashed lines correspond to one standard deviation of the curve parameter May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-055 EXCLUSIVE rho |
The same as 10-090 but after averaging over Q^{2} May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-054 EXCLUSIVE rho |
The dependences of |U_{11}/T_{00}| on Q^{2} and t' for proton and deuteron data. The points show the amplitude ratios after averaging over -t' binsl. The inner error bars show the statistical uncertainty and the outer ones show the statistical and systematic uncertainties added in quadrature. The results fitting the combined data set with a constant (central line), |U_{11}/T_{00}|=g, are shown. The dashed lines correspond to one standard deviation in the total uncertainty May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-053 EXCLUSIVE rho |
The same as 10-088 but for Im(T_{11}/T_{00}) / Q May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-052 EXCLUSIVE rho |
The t' dependence of Q* Re(T_{11}/T_{00}) for proton and deuteron data. Points show the amplitude ratios after averaging over four Q^{2} bins. The straight lines show the value of the fitted parameters. The meaning of the error bars and the explanation of the curves are the same as for 10-086 May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-051 EXCLUSIVE rho |
same as 10-086 but for \delta_{01} May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-050 EXCLUSIVE rho |
The Q^{2} dependence of the phase difference \delta_{11} (left panel) between the amplitudes T_{11} and T_{00} obtained for proton and deuteron data. Inner error bars show the statistical uncertainty and the outer ones show the statistical and systematic uncertainties added in quadrature. The fitted parameterization is also shown. The central lines are calculated with the fitted values of the parameters, while the dashed lines correspond to one standard deviation in the uncertainty of the curve parameter May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-049 EXCLUSIVE rho |
same as 10-84 but for Im( T_{11}/T_{00}) May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-048 EXCLUSIVE rho |
The Q^{2} dependence of Re(T_{11}/T_{00} for proton and deuteron data. Points show the amplitude ratios after averaging over four -t^' bins. The parameterization of the curves obtained from combined proton and deuteron data is also shown May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-047 EXCLUSIVE rho |
same as 10-082 but for deuteron May 10, 2011 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
S. Manaenkov
final |
11-046 EXCLUSIVE rho |
The Q^{2} dependence of Re( T_{11}/T_{00} ) for proton data, showing the result for the 16 (Q^{2}, -t') bins. Inner error bars show the statistical uncertainty and the total error bars represent statistical and systematic uncertainties added in quadrature. The data is fitted. Central lines are calculated with the fitted values of parameters, while the dashed lines correspond to one standard deviation of the curve parameter. Except for the second -t' bin, the data points are shifted for better visibility May 10, 2011 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
S. Manaenkov
final |
11-045 EXCLUSIVE rho |
Comparison of SDME and amplitude methods. Red squares show the results of the SDME analysis. Blue circles (amplitude method) are obtained in the present work from amplitude ratios fitted directly to the three-dimensional angular distribution in every Q^{2} and -t^' bin. The deuteron data at < Q^{2}> = 1.19 GeV^{2}, <-t'>= 0.145 GeV^{2} are presented. Yellow bands mark those SDMEs that are non-zero in the SCHC approximation. Total uncertainties are depicted May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-044 EXCLUSIVE rho |
Comparison of SDME and amplitude methods. Red squares show the results of the SDME analysis. Blue circles (amplitude method) are obtained in the present work from amplitude ratios fitted directly to the three-dimensional angular distribution in every Q^{2} and -t' bin. The proton data at < Q^{2} > = 3 GeV^{2}, < -t' > = 0.019 GeV^{2} are presented. Yellow bands mark those SDMEs that are non-zero in the SCHC approximation. Total uncertainties are depicted May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
11-043 EXCLUSIVE rho |
Definition of angles in the process eN -> e' rho^{0} N' -> e' pi^+ pi^- N'. Here Phi is the angle between the rho^{0} production plane and the lepton scattering plane in the CM system of virtual photon and target nucleon. The variables \theta and \phi are respectively the polar and azimuthal angles of the decay pi^+ in the rho^{0}-meson rest frame, with the Z axis being anti-parallel to the outgoing nucleon momentum May 10, 2011 *Colour (eps) *Colour (pdf) |
S. Manaenkov
final |
16-179 VECTOR-MESONS asymmetry, omega |
As Fig. 5, but only for transversely polarized omega mesons Jun 26, 2016 *Colour (eps) *Colour (pdf) *Data |
B. Marianski
final |
16-178 VECTOR-MESONS asymmetry, omega |
The five amplitudes describing the strength of the sine modulations of the cross section for hard exclusive omega meson production. The full circles show the data in two bins of Q^{2} or -t^{\prime}. The open squares represent the results obtained for the entire kinematic region. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature. The results receive an additional 8.2% scale uncertainty corresponding to the target-polarization uncertainty. The solid (dash-dotted) lines show the calculation of the GK model for a positive (negative) \pi\omega transition form factor, and the dashed lines are the model results without the pion pole Jun 26, 2016 *Colour (eps) *Colour (pdf) *Data |
B. Marianski
final |
16-177 VECTOR-MESONS asymmetry, omega |
Lepton-scattering and omega production planes together with the azimuthal angles \phi and \phi_{S} Jun 26, 2016 *Colour (eps) *Colour (pdf) |
B. Marianski
final |
16-176 VECTOR-MESONS asymmetry, omega |
The \pi^{+}\pi^{-}\pi^{0} invariant-mass distribution after application of all criteria to select exclusively produced omega mesons. The Breit-Wigner fit to the mass distribution is shown as a continuous line and the vertical dashed line indicates the PDG value of the omega mass Jun 26, 2016 *Colour (eps) *Colour (pdf) *Data |
B. Marianski
final |
16-175 VECTOR-MESONS asymmetry, omega |
Missing-energy distribution for exclusive omega meson production. The unshaded histogram shows experimental data, while the shaded area shows the distribution obtained from a PYTHIA simulation of the SIDIS background. The vertical dashed line denotes the upper limit of the exclusive region Jun 26, 2016 *Colour (eps) *Colour (pdf) |
B. Marianski
final |
16-174 VECTOR-MESONS asymmetry, omega |
Two-photon invariant-mass distribution after application of all criteria to select exclusively produced omega mesons. The Breit-Wigner fit to the mass distribution is shown as a continuous line and the vertical dashed line indicates the PDG value of the \pi^{0} mass Jun 26, 2016 *Colour (eps) *Colour (pdf) *Data |
B. Marianski
final |
14-045 VECTOR-MESONS omega spin density matrix elements |
The Q^{2} and -t^{\prime} dependences of the UPE-to-NPE asymmetry P of the transverse differential cross-section for exclusive \omega electroproduction at HERMES. The open symbols represent the values over the entire kinematic region Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-044 VECTOR-MESONS omega spin density matrix elements |
The Q^{2} (left) and -t^{\prime} (right) dependences of the longitudinal-to-transverse virtual photon differential cross-section ratio for exclusive \omega and \rho^{0} electroproduction at HERMES, where the -t^{\prime} bin covers the interval [0.0-0.2] GeV^{2} for \omega production and [0.0-0.4] GeV^{2} for \rho^{0} production. The symbols that are parenthesized in the legend represent the value of R in the entire kinematic region Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-043 VECTOR-MESONS omega spin density matrix elements |
The Q^{2} and -t^{\prime} dependences of u_{1},u_{2} and u_{3}. The open symbols represent the values over the entire kinematic region Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-042 VECTOR-MESONS omega spin density matrix elements |
Comparison of SDMEs in exclusive \omega and \rho^{0} electroproduction at HERMES for the entire kinematic region. The average values of the kinematic variables in exclusive \rho^{0} production are \left\langle Q^{2} \right\rangle = 1.95 GeV^{2}, \left\langle W \right\rangle = 4.8 GeV, and \left\langle -t^{\prime} \right\rangle = 0.13 GeV^{2} Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-041 VECTOR-MESONS omega spin density matrix elements |
Q^{2} and -t^{\prime} dependences of class-E SDMEs Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-040 VECTOR-MESONS omega spin density matrix elements |
-t^{\prime} dependence of class-D SDMEs Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-039 VECTOR-MESONS omega spin density matrix elements |
Q^{2} dependence of class-D SDMEs Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-038 VECTOR-MESONS omega spin density matrix elements |
-t^{\prime} dependence of class-C SDMEs Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-037 VECTOR-MESONS omega spin density matrix elements |
Q^{2} dependence of class-C SDMEs Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-036 VECTOR-MESONS omega spin density matrix elements |
Q^{2} and -t^{\prime} dependences of class-B SDMEs Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-035 VECTOR-MESONS omega spin density matrix elements |
Q^{2} and -t^{\prime} dependences of class-A SDMEs. Proton data are denoted by squares and deuteron data by circles. Data points for deuteron are slightly shifted horizontally for legibility Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-034 VECTOR-MESONS omega spin density matrix elements |
The 23 SDMEs for exclusive \omega electroproduction extracted in the entire HERMES kinematic region with \left\langle Q^{2} \right\rangle = 2.42 GeV^{2}, \left\langle W \right\rangle = 4.8 GeV, \left\langle -t^{\prime} \right\rangle = 0.080 GeV^{2}. Proton data are denoted by squares and deuteron data by circles. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature. Unpolarized (polarized) SDMEs are displayed in the unshaded (shaded) areas Jan 27, 2015 *Colour (eps) *Colour (pdf) *Data |
B. Marianski and A. Terkulov
final |
14-033 VECTOR-MESONS omega spin density matrix elements |
Distributions of several kinematic variables from experimental data on exclusive \omega meson leptoproduction (black squares) in comparison with simulated exclusive events from the PYTHIA generator (dashed areas). Simulated events are normalized to the experimental data Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-032 VECTOR-MESONS omega spin density matrix elements |
Distributions of several kinematic variables from experimental data on exclusive \omega meson leptoproduction (black squares) in comparison with simulated exclusive events from the PYTHIA generator (dashed areas). Simulated events are normalized to the experimental data Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-031 VECTOR-MESONS omega spin density matrix elements |
The \Delta E distribution of \omega mesons produced in the third -t^{\prime} kinematic bins is compared with SIDIS \Delta E distributions from PYTHIA (shaded area). The vertical dashed line denotes the upper limit of the exclusive region Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-030 VECTOR-MESONS omega spin density matrix elements |
The \Delta E distribution of \omega mesons produced in the second -t^{\prime} kinematic bins is compared with SIDIS \Delta E distributions from PYTHIA (shaded area). The vertical dashed line denotes the upper limit of the exclusive region Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-029 VECTOR-MESONS omega spin density matrix elements |
The \Delta E distribution of \omega mesons produced in the first -t^{\prime} kinematic bins is compared with SIDIS \Delta E distributions from PYTHIA (shaded area). The vertical dashed line denotes the upper limit of the exclusive region Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-028 VECTOR-MESONS omega spin density matrix elements |
The \Delta E distribution of \omega mesons produced in the entire kinematic region is compared with SIDIS \Delta E distributions from PYTHIA (shaded area). The vertical dashed line denotes the upper limit of the exclusive region Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-027 VECTOR-MESONS omega spin density matrix elements |
Breit-Wigner fit (solid line) of \pi^{+}\pi^{-}\pi^{0} invariant mass deistribution after application of all criteria to select \omega mesons produced exclusively from proton (top) and from deuteron (bottom). The dashed line represents the PDG value of the \omega mass Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-026 VECTOR-MESONS omega spin density matrix elements |
Two photon invariant mass distribution after application of all criteria to select exclusively produced \omega mesons. The Breit-Wigner fit to the mass distribution is shown as a continuous line and the dashed line indicates the PDG value of the \pi^{0} mass Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
14-025 VECTOR-MESONS omega spin density matrix elements |
Definition of angles in the process eN \rightarrow eN\omega, where \omega \rightarrow \pi^{+}\pi^{-}\pi^{0} Jan 27, 2015 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
final |
13-052 VECTOR-MESONS omega spin density matrix elements |
The longitudinal-to-transverse cross section ratio R_{L/T} as a function of Q^{2} for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-051 VECTOR-MESONS omega spin density matrix elements |
u3 as a function of t' for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-050 VECTOR-MESONS omega spin density matrix elements |
u3 as a function of Q^{2} for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-049 VECTOR-MESONS omega spin density matrix elements |
u2 as a function of t' for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-048 VECTOR-MESONS omega spin density matrix elements |
u2 as a function of Q^{2} for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-047 VECTOR-MESONS omega spin density matrix elements |
u1 as a function of t' for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-046 VECTOR-MESONS omega spin density matrix elements |
u1 as a function of Q^{2} for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-045 VECTOR-MESONS omega spin density matrix elements |
The class D SDMEs as a function of t' for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-044 VECTOR-MESONS omega spin density matrix elements |
The class D SDMEs as a function of Q^{2} for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-043 VECTOR-MESONS omega spin density matrix elements |
The class C SDMEs as a function of t' for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-042 VECTOR-MESONS omega spin density matrix elements |
The class C SDMEs as a function of Q^{2} for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-041 VECTOR-MESONS omega spin density matrix elements |
The class B SDMEs as a function of t' for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-040 VECTOR-MESONS omega spin density matrix elements |
The class B SDMEs as a function of Q^{2} for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-039 VECTOR-MESONS omega spin density matrix elements |
The class A SDMEs as a function of t' for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-038 VECTOR-MESONS omega spin density matrix elements |
The class A SDMEs as a function of Q^{2} for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-037 VECTOR-MESONS omega spin density matrix elements |
The t' dependence of the 23 SDMEs for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-036 VECTOR-MESONS omega spin density matrix elements |
The Q^{2} dependence of the 23 SDMEs for data collected on hydrogen and deuterium. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature Mar 19, 2013 *Colour (eps) *Colour (pdf) |
B. Marianski and A. Terkulov
prelim |
13-035 VECTOR-MESONS omega spin density matrix elements |
The 23 omega and rho SDMEs extracted from data collected on hydrogen and deuterium, in the entire HERMES kinematics with 2>=2.42 GeV^{2} and <-t'>=0.796 GeV^{2}. The SDMEs are multiplied by prefactors in order to represent the normalized leading contribution of the corresponding amplitude. SDMEs extracted with unpolarized (polarized) beam are displayed in the unshaded (shaded) areas. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature |
B. Marianski and A. Terkulov
prelim |
13-034 VECTOR-MESONS omega spin density matrix elements |
The 23 omega SDMEs extracted from data collected on hydrogen and deuterium, in the entire HERMES kinematics with 2>=2.42 GeV^{2} and <-t'>=0.796 GeV^{2}. SDMEs extracted with unpolarized (polarized) beam are displayed in the unshaded (shaded) areas. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature |
B. Marianski and A. Terkulov
prelim |
13-033 VECTOR-MESONS omega spin density matrix elements |
The 23 omega SDMEs extracted from data collected on hydrogen and deuterium, in the entire HERMES kinematics with 2>=2.42 GeV^{2} and <-t'>=0.796 GeV^{2}. The SDMEs are multiplied by prefactors in order to represent the normalized leading contribution of the corresponding amplitude. SDMEs extracted with unpolarized (polarized) beam are displayed in the unshaded (shaded) areas. The inner error bars represent the statistical uncertainties, while the outer ones indicate the statistical and systematic uncertainties added in quadrature |
B. Marianski and A. Terkulov
prelim |
09-015 VECTOR-MESONS asymmetry, omega |
Moments of the azimuthal target-spin asymmetry in exclusive electroproduction of omega mesons on a transversely polarized hydrogen target, in bins of -t', x-Bjorken and Q^{2}. The values integrated over the covered kinematic region are also given May 14, 2009 *Colour (eps) *Colour (pdf) INFO: The data points are contained in the data file attached to this entry. |
B. Marianski, S. Borissov, S. Manaenkov, W.-D. Nowak
prelim |
99-086 HIGH-PT |
A_{parallel} for pairs of high-p_{T} hadrons vs p_{T}^{h}+, with negative hadron leading (four panels) Jan 13, 2000 *BW (eps) *BW (pdf) |
J. Martin
final |
99-085a HIGH-PT |
A_{parallel} for pairs of high-p_{T} hadrons vs p_{T}^{h}+, with p_{T}^{h}- > 1.5 Jan 13, 2000 *BW (eps) *BW (pdf) |
J. Martin
final |
99-085b HIGH-PT |
A_{parallel} for pairs of high-p_{T} hadrons vs p_{T}^{h}-, with p_{T}^{h}+ > 1.5 Jan 13, 2000 *BW (eps) *BW (pdf) |
J. Martin
final |
99-084 HIGH-PT |
A_{parallel} for pairs of high-p_{T} hadrons vs p_{T}^{h2}, with p_{T}^{h1} > 1.5 Jan 13, 2000 *BW (eps) *BW (pdf) |
J. Martin
final |
99-083a HIGH-PT |
Data - Monte Carlo yield comparison for pairs of high-p_{T} hadrons vs p_{T}^{h}+, with p_{T}^{h}- > 1.5 Jan 13, 2000 *Colour (eps) *Colour (pdf) |
J. Martin
final |
99-083b HIGH-PT |
Data - Monte Carlo yield comparison for pairs of high-p_{T} hadrons vs p_{T}^{h}-, with p_{T}^{h}+ > 1.5 Jan 13, 2000 *Colour (eps) *Colour (pdf) |
J. Martin
final |
99-082 HIGH-PT |
Subprocess fractions contributing to production of pairs of high-p_{T} hadrons, according to PYTHIA model Jan 13, 2000 *Colour (eps) *Colour (pdf) |
J. Martin
final |
99-059 HIGH-PT |
A_{parallel} for high-p_{T} hadron pairs in 2 views: top (bottom) panel has positive (negative) hadron p_{T} > 1.5 1999 *BW (eps) *BW (pdf) |
J. Martin
final |
99-058 HIGH-PT |
Comparison of data and PYTHIA Monte Carlo for yield of hadron pairs vs p_{T}^{h2}, with p_{T}^{h1} > 1.5 1999 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
J. Martin
final |
99-057 HIGH-PT |
Measured A_{parallel} for hadrons pairs vs p_{T}^{h2}, overlaid with Monte Carlo predictions for various values of deltaG/G 1999 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
J. Martin
final |
99-056 HIGH-PT |
Best fit deltaG/G point vs x_{G}, overlaid with four theoretical parametrizations 1999 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) |
J. Martin
final |
99-049 DIAGRAM |
Feynman diagram of photon gluon fusion 1999 *Colour (eps) *Colour (pdf) |
J. Martin
final |
99-048 DIAGRAM |
Feynman diagram of the QCD Compton process 1999 *Colour (eps) *Colour (pdf) |
J. Martin
final |
99-047 DIAGRAM |
Feynman diagram of single quark scattering 1999 *Colour (eps) *Colour (pdf) |
J. Martin
final |
99-046 DIAGRAM |
Feynman diagram of vector meson dominance 1999 *Colour (eps) *Colour (pdf) |
J. Martin
final |
99-006 HIGH-PT |
Full slide describing PYTHIA model and method for extraction of deltaG/G from high p_{T} hadron pair asym 1999 *Colour *Colour (eps) *Colour (pdf) |
J. Martin
prelim |
09-089 DVCS deuterium |
The deuteron elastic form factors. See caption of Fig. 3 for more details Dec 10, 2009 *Colour (eps) *Colour (pdf) |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
09-088 DVCS deuterium |
The measured distribution of electroproduced real-photon events versus the squared missing mass M_{X}^{2}. The solid curve represents a Monte Carlo simulation. See caption of Fig. 4 for more details Dec 10, 2009 *Colour (eps) *Colour (pdf) |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
09-087 DVCS deuterium |
Distribution in the constrained Mandelstam variable t_{c} of events selected in the exclusive region of M_{X}^{2}. See caption of Fig. 5 for more details Dec 10, 2009 *Colour (eps) *Colour (pdf) |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
09-086 DVCS deuterium |
Amplitudes of the DVCS beam-charge asymmetry in 6 bins of -t_{c}, x_{N}, or Q^{2} on an unpolarized deuterium target. The error bars (bands) represent the statistical (systematic) uncertainties. Also included are VGG model calculations and the simulated fractions of coherent and resonant production in each kinematic bin Dec 10, 2009 *Colour (eps) *Colour (pdf) *Data INFO: The data values for each 6 kinematic bins are contained in the file attached to this entry. The data values for 4 kinematic bins (old binning) are attached to entry 09-085. |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
09-085 DVCS deuterium |
Leading amplitudes of the DVCS beam-helicity asymmetries in 6 bins of -t_{c}, x_{N}, or Q^{2} on an unpolarized deuterium target. The amplitude in the top row is sensitive to the squared DVCS term, while the amplitudes in the 2nd and 3rd row are sensitive to the Bethe-Heitler/DVCS interference term. There is an overall 2.4% scale uncertainty arising from the uncertainty in the measurement of the beam polarization. The error bars (bands) represent the statistical (systematic) uncertainties. Also included are VGG model calculations Dec 10, 2009 *Colour (eps) *Colour (pdf) *Data INFO: The data values (for 6 kinematic bins) are contained in the file attached to entry 09-086. The data values for each 4 kinematic bins are contained in the file attached to this entry. The 4-bins result is only given for completeness, while this publication only shows results for 6 kinematic bins. |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
09-084 DVCS deuterium |
The cos(0\phi) amplitudes of the DVCS beam-helicity asymmetries that are included as a consistency test in the maximum likelihood fit Dec 10, 2009 *Colour (eps) *Colour (pdf) INFO: Supportive plot. |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
09-083 DVCS deuterium |
Amplitudes of the DVCS beam-charge asymmetry in 6 bins of -t_{c}, x_{N}, or Q^{2} on an unpolarized deuterium target and on an unpolarized hydrogen target. The error bars (bands) represent the statistical (systematic) uncertainties Dec 10, 2009 *Colour (eps) *Colour (pdf) INFO: The deuterium values are contained in the data file attached to entry 09-089, while the hydrogen values are contained in the file attached to entry 09-071. |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
09-082 DVCS deuterium |
Amplitudes of the DVCS beam-helicity asymmetries that are sensitive to the squared DVCS term in 6 bins of -t_{c}, x_{N}, or Q^{2} on an unpolarized deuterium target and on an unpolarized hydrogen target. The error bars (bands) represent the statistical (systematic) uncertainties Dec 10, 2009 *Colour (eps) *Colour (pdf) INFO: The deuterium values are contained in the data file attached to entry 09-089, while the hydrogen values are contained in the file attached to entry 09-071. |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
09-081 DVCS deuterium |
Amplitudes of the DVCS beam-helicity asymmetries that are sensitive to the Bethe-Heitler/DVCS interference term in 6 bins of -t_{c}, x_{N}, or Q^{2} on an unpolarized deuterium target and on an unpolarized hydrogen target. The error bars (bands) represent the statistical (systematic) uncertainties Dec 10, 2009 *Colour (eps) *Colour (pdf) INFO: The deuterium values are contained in the data file attached to entry 09-089, while the hydrogen values are contained in the file attached to entry 09-071. |
H. Marukyan, G. Hill, C.A. Miller, A. Movsisyan
final |
08-044 DVCS deuterium |
The asymmetry amplitudes originating from the interference term extracted from all unpolarized deuterium data (1996-2005). The error bars (yellow bands) represent the statistical (systematic) uncertainties. The curves are predictions of a double-distribution model (blue and hatched bands indicating the range of varied parameters) or a polynomiality based model (black lines). The lowest panel shows the fractions of associated and coherent production, respectively (the first one being included only in the data but not in the MC used for the systematic studies) Nov 28, 2008 *Colour (eps) *Colour (pdf) INFO: Update after bugfix in VGG (c0) calculations. Dual curves removed. |
H. Marukyan and G. Hill
prelim |
08-044b DVCS deuterium |
The asymmetry amplitudes originating from the interference term extracted from all unpolarized deuterium data (1996-2005). The error bars (yellow bands) represent the statistical (systematic) uncertainties. The plot includes a comparison of a model with smearing & acceptance and a model at mean kinematics, of which the difference has been assigned as sytematic uncertainty. WARNING: the chosen model variant is considered to describe the HERMES data, but it is known to have a theoretical calculation error. This does however not affect this study, but only the interpretation in terms of GPDs. The lowest panel shows the fractions of associated and coherent production, respectively (the first one being included only in the data but not in the MC used for the systematic studies) Nov 28, 2008 *Colour (eps) *Colour (pdf) INFO: Supportive Plot. Reference to Dual curves removed. |
H. Marukyan and G. Hill
prelim |
08-043 DVCS deuterium |
The pure DVCS squared asymmetry amplitudes extracted from all unpolarized deuterium data (1996-2005). The error bars (bands) represent the statistical (systematic) uncertainties. The curves are predictions of a double-distribution model (blue and hatched bands indicating the range of varied parameters) or a polynomiality based model (black lines). The lowest panel shows the fractions of associated and coherent production, respectively (the first one being included only in the data but not in the MC used for the systematic studies) Nov 28, 2008 *Colour (eps) *Colour (pdf) INFO: Update after bugfix in VGG (c0) calculations. Dual curves removed. See record 08-044 for data tables. |
H. Marukyan and G. Hill
prelim |
08-043b DVCS deuterium |
The pure DVCS squared asymmetry amplitudes extracted from all unpolarized deuterium data (1996-2005). The error bars (bands) represent the statistical (systematic) uncertainties. The plot includes a comparison of a model with smearing & acceptance and a model at mean kinematics, of which the difference has been assigned as sytematic uncertainty. WARNING: the chosen model variant is considered to describe the HERMES data, but it is known to have a theoretical calculation error. This does however not affect this study, but only the interpretation in terms of GPDs. The lowest panel shows the fractions of associated and coherent production, respectively (the first one being included only in the data but not in the MC used for the systematic studies) Nov 28, 2008 *Colour (eps) *Colour (pdf) INFO: Supportive Plot. Reference to Dual curves removed. |
H. Marukyan and G. Hill
prelim |
08-042 DVCS deuterium |
The charge asymmetry amplitudes extracted from all unpolarized deuterium data (1996-2005). The error bars (bands) represent the statistical (systematic) uncertainties. The curves are predictions of a double-distribution model (blue and hatched bands indicating the range of varied parameters) or a polynomiality based model (black lines). The lowest panel shows the fractions of associated and coherent production, respectively (the first one being included only in the data but not in the MC used for the systematic studies) Nov 28, 2008 *Colour (eps) *Colour (pdf) INFO: Update after bugfix in VGG (c0) calculations. Dual curves removed. See record 08-044 for data tables. |
H. Marukyan and G. Hill
prelim |
08-042b DVCS deuterium |
The charge asymmetry amplitudes extracted from all unpolarized deuterium data (1996-2005). The error bars (bands) represent the statistical (systematic) uncertainties. The plot includes a comparison of a model with smearing & acceptance and a model at mean kinematics, of which the difference has been assigned as sytematic uncertainty. WARNING: the chosen model variant is considered to describe the HERMES data, but it is known to have a theoretical calculation error. This does however not affect this study, but only the interpretation in terms of GPDs. The lowest panel shows the fractions of associated and coherent production, respectively (the first one being included only in the data but not in the MC used for the systematic studies) Nov 28, 2008 *Colour (eps) *Colour (pdf) INFO: Supportive Plot. Reference to Dual curves removed. |
H. Marukyan and G. Hill
prelim |
08-041 DVCS proton, deuterium |
The asymmetry amplitudes originating from the interference term extracted from all data (1996-2005), comparing proton and unpolarized deuteron data. The error bars (bands) represent the statistical (systematic) uncertainties Aug 5, 2008 *Colour (eps) *Colour (pdf) |
H. Marukyan and G. Hill
prelim |
08-040 DVCS proton, deuterium |
The pure DVCS squared asymmetry amplitudes extracted from all data (1996-2005), comparing proton and unpolarized deuteron data. The error bars (bands) represent the statistical (systematic) uncertainties Aug 5, 2008 *Colour (eps) *Colour (pdf) INFO: Updated Dec 22, 2008: proton data points were missing in the 'overall' case. |
H. Marukyan and G. Hill
prelim |
08-039 DVCS proton, deuterium |
The charge asymmetry amplitudes extracted from all data (1996-2005), comparing proton and unpolarized deuteron data. The error bars (bands) represent the statistical (systematic) uncertainties Aug 5, 2008 *Colour (eps) *Colour (pdf) |
H. Marukyan and G. Hill
prelim |
01-009 VECTOR-MESONS asymmetry, rho |
Schematic graphs for exclusive rho^{0} production (a) and inclusive lepton-nucleon scattering (b) Feb 15, 2001 *Colour (eps) *Colour (pdf) |
F. Meissner
final |
01-008 VECTOR-MESONS asymmetry, rho |
Photon-nucleon asymmetry A_{1}^{rho} in exclusive rho^{0} production versus theta. Error bars and error bands denote the statistical and experimental systematic uncertainties, respectively Feb 15, 2001 *Colour (eps) *Colour (pdf) |
F. Meissner
final |
01-007 VECTOR-MESONS asymmetry, rho |
Photon-nucleon asymmetry A_{1}^{rho} in exclusive rho^{0} production versus Phi. Error bars and error bands denote the statistical and experimental systematic uncertainties, respectively Feb 15, 2001 *Colour (eps) *Colour (pdf) |
F. Meissner
final |
01-006 VECTOR-MESONS asymmetry, rho |
Photon-nucleon asymmetry A_{1}^{rho} in exclusive rho^{0} production versus -t'. Error bars and error bands denote the statistical and experimental systematic uncertainties, respectively Feb 15, 2001 *Colour (eps) *Colour (pdf) |
F. Meissner
final |
01-005 VECTOR-MESONS asymmetry, rho |
Photon-nucleon asymmetry A_{1}^{rho} in exclusive rho^{0} production versus x. Error bars and error bands denote the statistical and experimental systematic uncertainties, respectively Feb 15, 2001 *Colour (eps) *Colour (pdf) |
F. Meissner
final |
01-004 VECTOR-MESONS asymmetry, rho |
Photon-nucleon asymmetry A_{1}^{rho} in exclusive rho^{0} production versus W. Error bars and error bands denote the statistical and experimental systematic uncertainties, respectively Feb 15, 2001 *Colour (eps) *Colour (pdf) |
F. Meissner
final |
01-003 VECTOR-MESONS asymmetry, rho |
Photon-nucleon asymmetry A_{1}^{rho} in exclusive rho^{0} production versus Q^{2}. Error bars and error bands denote the statistical and experimental systematic uncertainties, respectively Feb 15, 2001 *Colour (eps) *Colour (pdf) *Data |
F. Meissner
final |
01-002 VECTOR-MESONS asymmetry, rho |
Distribution in the excitation energy Delta E for the decay channel rho^{0} to pi^+ pi^-, after all other event selection criteria were applied. The histogram is a Monte Carlo simulation of combinatorial background from deep-inelastic scattering (DIS). The shaded area indicates the events that were used for the analysis Feb 15, 2001 *Colour (eps) *Colour (pdf) |
F. Meissner
final |
01-001 VECTOR-MESONS asymmetry, rho |
Schematic graphs for various models of exclusive diffractive rho^{0} production: a) Reggeon or Pomeron exchange in models based on Regge theory, b) two-gluon exchange and c) quark exchange in models inspired by perturbative QCD Feb 15, 2001 *Colour (eps) *Colour (pdf) |
F. Meissner
final |
99-015 VECTOR-MESONS asymmetry |
A_{1} for the rho, phi, and J/psi (Note that the rho and phi data are from electroproduction, the J/psi is from quasi-real photoproduction) 1999 *Colour *Colour (eps) *Colour (pdf) |
F. Meissner
prelim |
98-067 CHARM j/psi |
J/Psi photoproduction cross section in comparison to other measurements at low E_{gamma} 1998 *Colour *Colour (eps) *Colour (pdf) |
F. Meissner
prelim |
98-066 CHARM j/psi |
J/Psi leptoproduction cross section from J/Psi-->e+e- and J/Psi-->mu+mu- 1998 *Colour *Colour (eps) *Colour (pdf) |
F. Meissner
prelim |
98-065 CHARM j/psi |
J/psi distributions (p_{e},omega,E_{J}/psi,p_{t}**2) for mu+mu- decay channel in comparsion to MC 1998 *Colour *Colour (eps) *Colour (pdf) |
F. Meissner
prelim |
98-064 CHARM j/psi |
J/psi distributions (p_{e},omega,E_{J}/psi,p_{t}**2) for e+e- decay channel in comparsion to MC 1998 *Colour *Colour (eps) *Colour (pdf) |
F. Meissner
prelim |
98-023 CHARM j/psi |
Preliminary J/Psi signal from 95-97 data (e+e- and mu+mu- decay channels) 1998 *Colour *Colour (eps) *Colour (pdf) |
F. Meissner
prelim |
98-022 CHARM j/psi |
Preliminary J/Psi signal from 95-97 data (e+e- decay channels) 1998 *Colour *Colour (eps) *Colour (pdf) |
F. Meissner
prelim |
98-021 CHARM j/psi |
Preliminary J/Psi signal from 95-97 data (mu+mu- decay channels) 1998 *Colour *Colour (eps) *Colour (pdf) |
F. Meissner
prelim |
96-105a DIAGRAM |
Diagram of open charm production via photon gluon fusion Feb 3, 2000 *BW (eps) *BW (pdf) *BW (fig) |
A. Miller
final |
96-105b DIAGRAM |
Diagram of hidden charm production via photon gluon fusion Feb 3, 2000 *BW (eps) *BW (pdf) *BW (fig) |
A. Miller
final |
96-105c DIAGRAM |
Diagram of diffractive J/psi production Feb 3, 2000 *BW (eps) *BW (pdf) *BW (fig) |
A. Miller
final |
14-010 DVCS associated |
Amplitudes of the single-charge beam-helicity asymmetry extracted in the associated channel ep->e\gammapi+n obtained with recoil-proton reconstruction. The amplitudes are presented in projections of -t, xB, and Q^{2}. The "overall" results shown in the very left panel are extracted in a single kinematic bin covering the entire kinematic acceptance. Statistical (systematic) uncertainties are represented by error bars (bands). A separate scale uncertainty arising from the measurement of the beam polarization amounts to 1.96% Jan 27, 2014 *Colour (eps) *Colour (pdf) *Data |
A. Movsisyan, S. Yaschenko
final |
14-009 DVCS associated |
Amplitudes of the single-charge beam-helicity asymmetry extracted in the associated channel ep->e\gammapi0p obtained with recoil-proton reconstruction. The amplitudes are presented in projections of -t, xB, and Q^{2}. The "overall" results shown in the very left panel are extracted in a single kinematic bin covering the entire kinematic acceptance. Statistical (systematic) uncertainties are represented by error bars (bands). A separate scale uncertainty arising from the measurement of the beam polarization amounts to 1.96% Jan 27, 2014 *Colour (eps) *Colour (pdf) *Data |
A. Movsisyan, S. Yaschenko
final |
14-008 DVCS associated |
Distributions of Q^{2} for the associated channel ep->e\gammapi+n. Notations are the same as in figure 1 Jan 27, 2014 *Colour (eps) *Colour (pdf) |
A. Movsisyan, S. Yaschenko
final |
14-007 DVCS associated |
Distributions of xB for the associated channel ep->e\gammapi+n. Notations are the same as in figure 1 Jan 27, 2014 *Colour (eps) *Colour (pdf) |
A. Movsisyan, S. Yaschenko
final |
14-006 DVCS associated |
Distributions of t for the associated channel ep->e\gammapi+n. Notations are the same as in figure 1 Jan 27, 2014 *Colour (eps) *Colour (pdf) |
A. Movsisyan, S. Yaschenko
final |
14-005 DVCS associated |
Distributions of Q^{2} for the associated channel ep->e\gammapi0p. Notations are the same as in figure 1 Jan 27, 2014 *Colour (eps) *Colour (pdf) |
A. Movsisyan, S. Yaschenko
final |
14-004 DVCS associated |
Distributions of xB for the associated channel ep->e\gammapi0p. Notations are the same as in figure 1 Jan 27, 2014 *Colour (eps) *Colour (pdf) |
A. Movsisyan, S. Yaschenko
final |
14-003 DVCS associated |
Distributions of t for the associated channel ep->e\gammapi0p. Notations are the same as in figure 1 Jan 27, 2014 *Colour (eps) *Colour (pdf) |
A. Movsisyan, S. Yaschenko
final |
14-002 DVCS associated |
Distribution of chi^{2}(ep->e\gamma\pi+n) for the channel ep->e\gamma\pi+n. Experimental data are presented by points, and the results of the Monte Carlo simulation by lines. Contributions from the associated, ep-> e\gammap, and SIDIS reactions are shown by red dash-dotted, blue dashed, and green dotted lines, respectively. Data and Monte Carlo yields are normalized to the corresponding numbers of DIS events Jan 27, 2014 *Colour (eps) *Colour (pdf) |
A. Movsisyan, S. Yaschenko
final |
14-001 DVCS associated |
Distribution of chi^{2}(ep->e\gamma\pi0p) for the channel ep->e\gamma\pi0p. Experimental data are presented by points, and the results of the Monte Carlo simulation by lines. Contributions from the associated, ep-> e\gammap, and SIDIS reactions are shown by red dash-dotted, blue dashed, and green dotted lines, respectively. Data and Monte Carlo yields are normalized to the corresponding numbers of DIS events Jan 27, 2014 *Colour (eps) *Colour (pdf) |
A. Movsisyan, S. Yaschenko
final |
11-086 DVCS proton |
Correlation matrix for all fitted asymmetry amplitudes. The closed symbols represent positive values, while the open ones are for negative values. The area of the symbols represents the size of the correlation Sep 17, 2011 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
A. Movsisyan, H. Marukyan
final |
11-085 DVCS proton |
Charge-averaged double-spin asymmetry amplitudes describing the dependence of the sum of squared DVCS and BH terms on transverse target polarization in combination with beam helicity extracted from hydrogen target data. The error bars (bands at the bottom of the panels) represent the statistical (systematic) uncertainties. There is an additional overall 8.6 % scale uncertainty arising from the uncertainties in the measurements of the beam and target polarizations. The curves and the bottom row of panels have the same meaning as in 11-084 Sep 17, 2011 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to the entry 11-084. |
A. Movsisyan, H. Marukyan
final |
11-084 DVCS proton |
Charge-difference double-spin asymmetry amplitudes describing the dependence of the interference term on transverse target polarization in combination with beam helicity and beam charge extracted from hydrogen target data. The error bars (bands at the bottom of the panels) represent the statistical (systematic) uncertainties. There is an additional overall 8.6 % scale uncertainty arising from the uncertainties in the measurements of the beam and target polarizations. The curves show the results of theoretical calculations using the VGG double-distribution model with a Regge ansatz for modeling the t dependence of GPDs. The widths of the curves represent the effect of varying the total angular momentum J_{u} of u-quarks between 0.2 and 0.6, with J_{d}=0. The bottom row shows the fractional contribution of associated BH production as obtained from a MC simulation Sep 17, 2011 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in the file attached to this entry. |
A. Movsisyan, H. Marukyan
final |
11-083 DVCS proton |
Momenta and azimuthal angles for exclusive real-photon electroproduction in the target rest frame. The quantity phi denotes the angle between the lepton scattering plane containing the three-momenta k and k' of the incoming and outgoing lepton and the photon production plane correspondingly defined by the vector q=k-k' and the momentum q' of the real photon. The symbol phi_{S} denotes the angle between the lepton scattering plane and S_\perp , the component of the target polarization vector that is orthogonal to q . These definitions are consistent with the Trento conventions Sep 17, 2011 *Colour (eps) *Colour (pdf) |
A. Movsisyan, H. Marukyan
final |
10-064 DVCS deuterium |
Results from the present work (red filled squares) representing single-charge beam-helicity asymmetry amplitudes describing the dependence of the sum of squared DVCS and interference terms on the beam helicity, for a tensor polarization of P_{zz}=0.827 . The black open squares represent charge-difference amplitudes from only the interference term, extracted from unpolarized deuterium data. The error bars represent the statistical uncertainties, while the coarsely hatched (open) bands represent the systematic uncertainties of the filled (open) squares. There is an additional overall 1.9% (2.4%) scale uncertainty arising from the uncertainty in the measurement of the beam polarization in the case of polarized (unpolarized) deuterium data. The points for unpolarized deuterium data are slightly shifted to the left for better visibility. The finely hatched band shows the results of theoretical calculations for the combination of incoherent scattering on proton and neutron, using variants of the VGG double-distribution model with a Regge ansatz for modeling the t dependence of GPDs Sep 17, 2010 *Colour (eps) *Colour (pdf) *Data INFO: The data values are contained in this entry. |
A. Movsisyan, H. Marukyan
final |
10-063 DVCS deuterium |
Simulated yield fractions of coherent and resonant production Sep 17, 2010 *Colour (eps) *Colour (pdf) |
A. Movsisyan, H. Marukyan
final |
10-062 DVCS deuterium |
Single-charge target-spin asymmetry amplitudes describing the dependence of the sum of squared DVCS and interference terms on the target vector polarization, for a tensor polarization of P_{zz}=0.827. The squares represent the results from the present work. The triangles denote the corresponding amplitudes extracted from longitudinally polarized hydrogen data. The error bars (bands) represent the statistical (systematic) uncertainties. The finely hatched bands have the same meaning as in 10-064. There is an additional overall 4.0% (4.2%) scale uncertainty arising from the uncertainty in the measurement of the target polarization in the case of deuterium (hydrogen). The points for hydrogen are slightly shifted to the left for better visibility Sep 17, 2010 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 10-064. |
A. Movsisyan, H. Marukyan
final |
10-061 DVCS deuterium |
Single-charge double-spin asymmetry amplitudes describing the dependence of the sum of Bethe-Heitler, squared DVCS and interference terms on the product of the beam helicity and target vector polarization, for a tensor polarization of P_{zz}=0.827. The plotted symbols and bands have the same meaning as in 10-060. There is an additional overall 4.4% (5.3%) scale uncertainty arising from the uncertainties in the measurement of the beam and target polarizations in the case of deuterium (hydrogen) data Sep 17, 2010 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 10-064. |
A. Movsisyan, H. Marukyan
final |
10-060 DVCS deuterium |
Results representing single-beam-helicity charge asymmetry amplitudes (red filled squares) for P_{ell}=-0.530 and a tensor polarization of P_{zz}=0.827. The black open squares are A_{C}^{\cos(n\phi)} amplitudes extracted from data recorded with an unpolarized beam and unpolarized deuterium target. The error bars and bands and finely hatched bands have the same meaning as in 10-060. The points for unpolarized deuterium data are slightly shifted to the left for better visibility. There is an additional overall 2.2% scale uncertainty arising from the uncertainty in the measurement of the beam polarization Sep 17, 2010 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 10-064. |
A. Movsisyan, H. Marukyan
final |
10-059 DVCS deuterium |
Kinematic dependence of the charge-averaged single-beam-helicity target-spin asymmetry amplitudes for P_{ell}=-0.530 and a tensor polarization of P_{zz}=0.827. The plotted symbols and bands have the same meaning as in 10-060. There is an additional overall 5.3% (5.7%) scale uncertainty for the extracted amplitudes arising from the uncertainties in the measurement of the target (beam and target) polarizations Sep 17, 2010 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 10-064. |
A. Movsisyan, H. Marukyan
final |
10-058 DVCS deuterium |
Kinematic dependence of the single-beam-helicity beam-charge $\otimes$ target-spin asymmetry amplitudes for P_{ell}=-0.530 and a tensor polarization of P_{zz}=0.827. The plotted symbols and bands have the same meaning as in 10-060. There is an additional overall 5.3% (5.7%) scale uncertainty for the extracted amplitudes arising from the uncertainties in the measurement of the target (beam and target) polarizations Sep 17, 2010 *Colour (eps) *Colour (pdf) INFO: The data values are contained in the file attached to entry 10-064. |
A. Movsisyan, H. Marukyan
final |
03-105 HADRON-ATTENUATION |
Multiplicity ratio for charged hadrons as a function of pt^{2} for z > 0.2 and nu > 7 GeV. Target: Krypton and Nitrogen Oct 10, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
V.Muccifora
final |
03-104 HADRON-ATTENUATION |
Multiplicity ratio for identified pions, kaons, protons and antiprotons as a function of z for nu > 7 GeV. Target: Krypton Oct 10, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
V.Muccifora
final |
03-103 HADRON-ATTENUATION |
Multiplicity ratio for identified pions, kaons, protons and antiprotons as a function of nu for z > 0.2 Target: Krypton Oct 10, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
V.Muccifora
final |
03-102 HADRON-ATTENUATION |
Charged hadron multiplicity ratio R_{M}^{h} as a function of z for nu > 7. GeV. Targets: Krypton and Nitrogen Oct 10, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
V.Muccifora
final |
03-101 HADRON-ATTENUATION |
Charged hadron multiplicity ratio R_{M}^{h} as a function of nu for z > 0.2. Targets: Krypton and Nitrogen Oct 10, 2003 *Colour (eps) *BW (eps) *Colour (pdf) *BW (pdf) *Data |
V.Muccifora
final |
03-100 HADRON-ATTENUATION |
kinematic plan for hadron production in semi-inclusive DIS Oct 10, 2003 *BW (eps) *BW (pdf) |
V.Muccifora
final |
00-090 HADRON-ATTENUATION |
Multiplicity ratios for hadrons including pions (top panel) and identified pions (bottom panel) as a function of nu. The open (closed) squares represent the positive (negative) hadrons. Identified pions are represented by open (positive) and closed (negative) circles. The curves are parameterizations of the data using the one time-scale model assuming t_{f}^{h} = c_{h} (1-z)nu Dec 21, 2000 *BW (eps) *BW (pdf) |
V. Muccifora
final |
00-089 HADRON-ATTENUATION |
The multiplicity ratio as a function of nu for charged pions with z greater than 0.5. The solid curve represents a gluon-bremsstrahlung model calculation. The dotted curve is the result of a one time-scale model calculation assuming a (1-z)nu-dependence of the formation time Dec 21, 2000 *BW (eps) *BW (pdf) |
V. Muccifora
final |
00-088 HADRON-ATTENUATION |
The multiplicity ratio as a function of z for all charged pions (open circles) and all charged hadrons including pions (closed squares). The full curve represents a gluon-bremsstrahlung model calculation for pions. The dotted, dashed and dot-dashed curves represent phenomenological formation-time calculations Dec 21, 2000 *BW (eps) *BW (pdf) |
V. Muccifora
final |
00-087 HADRON-ATTENUATION |
Charged hadron multiplicity ratio R_{M}^{h} as a function of nu for values of z larger than 0.2. In the upper panel the CERN and SLAC data for Cu are compared to various phenomenological calculations taken from the original publications. In the lower panel the HERMES data on nitrogen are represented by solid squares, while the open star represents the CERN data point on carbon and the open square the SLAC data point on carbon. The error bars represent the statistical uncertainty only. The systematic uncertainty of the HERMES data is less than 3 percent. The curves are described in the publication Dec 21, 2000 *BW (eps) *BW (pdf) |
V. Muccifora
final |
00-086 HADRON-ATTENUATION |
Scatter plot of the hadron (or pion) energy E_{h} (E_{pi}) and the energy transfer nu. Lines representing constant values of z are shown as well Dec 21, 2000 *BW (eps) *BW (pdf) |
V. Muccifora
final |
Author: N | ||