# Elastic and proton-dissociative photoproduction of J/psi mesons at HERA # [arXiv:1304.5162] # and # Diffractive Photoproduction of J/psi Mesons with Large Momentum Transfer at HERA # [hep-ex/0306013] # # In this document, the differential cross sections as a function of t # are given for the high energy dataset together with a decomposition # of the error matrix. Additional points from an older measurements, # extending the reach in t, are also included # # The table has 27 rows, corresponding to 27 cross section # measurements. Each row has 23 columns, as explained below. # Rows 1-17 correspond to table 5 of [arXiv:1304.5162]. # Rows 18-27 correspond to table 1 of [hep-ex/0306013]. # # Version 1, date: 20.6.2013 # Version 2, date: 7.2.2016 [fixed typo in row 6, column 'tavg'] # # Column 1-8: differential cross section measurement # column comment # ===================== # 1 (n) row number # 2 (pd) pd=0 if the reaction is elastic, pd=1 if proton dissociative # 3 (|tmin|) lower bound on the modulus of the momentum transfer [GeV^2] # 4 (|tmax|) upper bound on the modulus of the momentum transfer [GeV^2] # 5 (|tavg|) average modulus of the momentum transfer [GeV^2] # 6 (PhiT) transverse polarized photon flux # 7 (sigm) measured differential cross section [nanobarn/GeV^2] # 8 (dsig) total uncertainty on the differential cross section [nanobarn/GeV^2] # # Column 9-22: error sources # column comment # =================== # 9 (dunc) uncorrelated uncertainty [nanobarn/GeV^2] # 10 (dc1) 1st correlated uncertainty from data combination [nanobarn/GeV^2] # 11 (dc2) 2nd correlated uncertainty from data combination [nanobarn/GeV^2] # 12 (dc3) 3rd correlated uncertainty from data combination [nanobarn/GeV^2] # 13 (dc4) 4th correlated uncertainty from data combination [nanobarn/GeV^2] # 14 (dc5) 5th correlated uncertainty from data combination [nanobarn/GeV^2] # 15 (rnor) normalisation uncertainty from trigger, track and psi(2S) [percent] # 16 (rlhe) luminosity uncertainty for this (high energy) data set [percent] # 17 (rlar) LAr tagging uncertainty [percent] # 18 (rplu) PLUG tagging uncertainty [percent] # 19 (rfts) FTS tagging uncertainty [percent] # 20 (rmod) model uncertainty [percent] # 21 (rq2) Q^2 dependence uncertainty [percent] # 22 (rec) empty calorimeter cut uncertainty [percent] # 23 (rhe1) hera 1 data correlated uncertainty [percent] # # Note 1: the uncertainties from col=8 to col=14 are absolute uncertainties # measured in nanobarn/GeV^2, whereas the uncertainties from col=15 to col=23 # are given in percent, relative to col=7. # # Note 2: when adding all uncertainty sources corresponding col=9 up to # col=23 quadratically, the result is equal to the total uncertainty # given in col=8 (sanity check). # # Note 3: the uncertainties given in col=10 up to col=23 are correlated # across the rows of the table, i.e. they contribute to the # off-diagonals of the covariance matrix. In contrast, the # uncertainties given in col=9 are uncorrelated, so they contribute only # to the diagonals of the covariance matrix. # #n pd tmin tmax tavg PhiT sigm dsig dunc dc1 dc2 dc3 dc4 dc5 rnor rlhe rlar rplu rfts rmod rq2 rec rhe1 #================================================================================================================================= 1 0 0.00 0.05 0.02 0.0953 336.0 18.4 6.2 8.8 -2.3 0.5 0.1 0.0 3.2 2.7 -1.0 0.2 -0.1 -0.6 -0.1 0.5 0. 2 0 0.05 0.11 0.08 0.0953 240.5 12.9 4.9 4.2 3.2 0.7 -0.1 -0.1 3.2 2.7 -1.2 0.3 -0.1 -0.7 -0.1 0.6 0. 3 0 0.11 0.17 0.14 0.0953 161.2 9.3 4.4 2.6 1.9 -0.4 0.3 0.2 3.2 2.7 -1.6 0.3 -0.1 -1.0 -0.1 0.8 0. 4 0 0.17 0.25 0.21 0.0953 111.4 7.0 2.0 2.0 0.1 -3.0 0.1 0.0 3.2 2.7 -2.2 0.5 -0.1 -1.4 -0.1 1.0 0. 5 0 0.25 0.35 0.30 0.0953 70.4 5.1 2.7 1.2 0.1 -0.2 -1.0 -0.5 3.2 2.7 -2.9 0.6 -0.2 -1.9 -0.1 1.4 0. 6 0 0.35 0.49 0.41 0.0953 41.2 3.7 1.8 0.7 0.2 0.1 -1.0 0.3 3.2 2.7 -4.6 1.0 -0.3 -3.0 0.0 2.3 0. 7 0 0.49 0.69 0.58 0.0953 18.00 2.74 0.97 0.32 0.08 -0.05 -0.23 0.92 3.2 2.7 -9.2 2.1 -0.6 -6.5 0.1 4.7 0. 8 0 0.69 1.2 0.9 0.0953 4.83 1.75 0.63 0.08 0.02 0.01 0.04 0.20 3.2 2.7 -24.0 5.8 -1.4 -18.0 0.8 13.0 0. 9 1 0.0 0.2 0.1 0.0953 47.3 6.7 2.1 0.5 -0.0 -0.3 -0.8 0.2 3.2 2.7 11.0 -2.2 0.6 3.6 -0.1 -4.6 0. 10 1 0.2 0.4 0.29 0.0953 43.8 6.0 1.6 0.7 0.3 0.3 0.6 0.3 3.2 2.7 11.0 -2.4 0.6 2.2 -0.0 -4.7 0. 11 1 0.4 0.64 0.52 0.0953 36.7 5.1 1.3 0.6 0.3 -0.1 0.5 -0.4 3.2 2.7 11.0 -2.6 0.7 2.0 -0.1 -5.0 0. 12 1 0.64 0.93 0.78 0.0953 27.8 4.2 1.0 0.5 0.2 -0.2 -0.2 -0.6 3.2 2.7 12.0 -2.9 0.7 2.8 -0.1 -5.7 0. 13 1 0.93 1.31 1.12 0.0953 16.80 2.59 0.82 0.23 0.07 -0.05 -0.13 -0.05 3.2 2.7 12.0 -3.1 0.7 2.0 -0.1 -5.9 0. 14 1 1.31 1.83 1.55 0.0953 10.05 1.56 0.47 0.20 0.07 -0.03 -0.06 0.05 3.2 2.7 12.0 -3.1 0.5 1.7 0.0 -6.2 0. 15 1 1.83 2.63 2.21 0.0953 6.04 0.68 0.31 0.11 0.04 -0.02 -0.03 0.01 3.2 2.7 6.0 -1.7 0.3 -5.5 0.5 -3.0 0. 16 1 2.63 4.13 3.30 0.0953 2.80 0.38 0.15 0.04 0.01 -0.01 -0.01 0.00 3.2 2.7 6.7 -1.9 0.3 -8.7 0.5 -3.6 0. 17 1 4.13 8.0 5.71 0.0953 0.875 0.178 0.047 0.039 0.015 -0.006 -0.010 0.004 3.2 2.7 9.0 -2.5 0.3 -15.0 0.2 -5.4 0. 18 1 2.0 3.0 2.43 0.0000 4.753 0.663 0.270 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 12.7 19 1 3.0 4.0 3.45 0.0000 2.871 0.422 0.214 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 12.7 20 1 4.0 5.0 4.46 0.0000 1.370 0.218 0.140 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 12.2 21 1 5.0 6.0 5.47 0.0000 0.811 0.152 0.112 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 12.6 22 1 6.0 7.0 6.47 0.0000 0.569 0.115 0.092 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 12.1 23 1 7.0 9.0 7.92 0.0000 0.266 0.053 0.043 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 11.9 24 1 9.0 12. 10.4 0.0000 0.141 0.029 0.024 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 11.3 25 1 12.0 15. 13.4 0.0000 0.087 0.021 0.019 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 10.8 26 1 15.0 21. 17.7 0.0000 0.0220 0.0067 0.0062 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 11.4 27 1 21.0 30. 25.0 0.0000 0.0042 0.0022 0.0021 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 11.1