cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.44217.v1/t18
title: "Table 18" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The slope of the RHO0 dsig/dt distribution from the DIS data. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t19
title: "Table 19" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The slope of the RHO0 dsig/dt distribution from the DIS data. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t20
title: "Table 20" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The slope of the RHO0 dsig/dt distribution from the DIS data. The second systematic (DSYS) error is the uncertainty arising from the subtraction of the proton dissiciation background.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t21
title: "Table 21" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 BPC sample.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t22
title: "Table 22" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 BPC sample.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t23
title: "Table 23" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 DIS sample.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t24
title: "Table 24" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 DIS sample.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t25
title: "Table 25" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: Ratio of the cross sections for longitudinal and transverse photons from the DIS data as a function of Q**2.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t26
title: "Table 26" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: Ratio of the cross sections for longitudinal and transverse photons from the BPC data as a function of Q**2.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t27
title: "Table 27" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: Ratio of the cross sections for longitudinal and transverse photons from the BPC data as a function of W.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t28
title: "Table 28" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: Ratio of the cross sections for longitudinal and transverse photons from the DIS data as a function of W.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t29
title: "Table 29" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The measured forward longitudinal cross section as a function of x for the DIS RHO0 data sample. NOTE FROM THE AUTHORS about figure 19_21:. Please note that the positive and negative error bars in the publication Eur.Phys.J. C6 (1999) 603 were inadvertently exchanged. In this table we give thetotal systematic uncertainty on each point as the quadratic sum of the correlat ed systematic error, shown as shaded bands in the publication, and the systematic error bars.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t30
title: "Table 30" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The measured forward longitudinal cross section as a function of x for the DIS RHO0 data sample. See note above from the authors.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t31
title: "Table 31" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The measured forward longitudinal cross section as a function of x for the DIS RHO0 data sample. See note above from the authors.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44217.v1/t32
title: "Table 32" of "Exclusive electroproduction of rho0 and J / psi mesons at HERA"

description: The measured forward longitudinal cross section as a function of x for the DIS RHO0 data sample. See note above from the authors.
description: DESY-HERA. Measurement of the exclusive production of RHO0 and J/PSI mesonsin positron-proton interactions at cm energy of 300 GeV. Data are collected at low Q**2 for RHO0 production using the Beam Pipe Calorimeter (BPC) and at higherQ**2 for both meson types (the DIS data sample). Cross sections and spin-densit ymatrices are determined from the data.. Numerical values of figures 16, 18 and 19_21 supplied by J Crittenden.
DOI: 10.17182/hepdata.44218.v1/t1
title: "Table 1" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t2
title: "Table 2" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t10
title: "Table 10" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t3
title: "Table 3" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t4
title: "Table 4" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t5
title: "Table 5" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t6
title: "Table 6" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t7
title: "Table 7" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t8
title: "Table 8" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t11
title: "Table 11" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t12
title: "Table 12" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t13
title: "Table 13" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: Total cross section as a function of the GAMMA P invariant mass W and virtual photon polarization EPS obtained using General Vector Meson Dominance (GVMD) extrapolation and assumption SIG_L = 0.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t14
title: "Table 14" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: Values of slope D(LN(F2))/D(1/X) calculated from fitting F2 = A*X**(-SLOPE)to ZEUS + E665 data.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t15
title: "Table 15" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: Values of slope D(F2)/D(LN(Q2)) calculated from fitting F2 = A + B*LN(Q2) to the ZEUS data.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44218.v1/t9
title: "Table 9" of "ZEUS results on the measurement and phenomenology of F2 at low x and low Q**2."

description: F2.
description: DESY-HERA. Measurement of the proton structure function, F2, for 0.6 & lt; Q2 & lt;17 GeV**2 and 1.2*10-5 & lt; x & lt; 1.9*10-3 from the ZEUS 1995 shifted vertex (SV X95 ) run. Data also include the total cross section as a function of the virtual photon c.m. energy, and the slope of F2 as functions of both Q**2 at fixed X and ln(1/X) at fixed Q**2.
DOI: 10.17182/hepdata.44219.v1/t1
title: "Table 1" of "Measurement of inclusive D*+- and associated dijet cross sections in photoproduction at HERA."

description: Integrated D*+- cross sections from the decay channel (1) AND (2).
description: DESY-HERA. Differential cross-sections of D*(2010)+- and associated dijet photoproduction in E P collisions at HERA. The variable XOBS(C=GAMMA) is deined as:. (E(jet1)*EXP(-ETARAP(jet1)) + E(jet2)*EXP(-ETARAP(jet2)))/(2*Y*E_e). and is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: and Y = E_gamma/E_e. Decay Channel (1) is D*+ --& gt; D0 PI+s --& gt; (K- PI+) PI+s and CC. Decay Channel (2) is D*+ --& gt; D0 PI+ --& gt; (K- PI+ PI+ PI-) PI+s and CC.
DOI: 10.17182/hepdata.44219.v1/t2
title: "Table 2" of "Measurement of inclusive D*+- and associated dijet cross sections in photoproduction at HERA."

description: Differential cross section, as a function of transverse momentum, from decay channel (1).
description: DESY-HERA. Differential cross-sections of D*(2010)+- and associated dijet photoproduction in E P collisions at HERA. The variable XOBS(C=GAMMA) is deined as:. (E(jet1)*EXP(-ETARAP(jet1)) + E(jet2)*EXP(-ETARAP(jet2)))/(2*Y*E_e). and is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: and Y = E_gamma/E_e. Decay Channel (1) is D*+ --& gt; D0 PI+s --& gt; (K- PI+) PI+s and CC. Decay Channel (2) is D*+ --& gt; D0 PI+ --& gt; (K- PI+ PI+ PI-) PI+s and CC.
DOI: 10.17182/hepdata.44219.v1/t3
title: "Table 3" of "Measurement of inclusive D*+- and associated dijet cross sections in photoproduction at HERA."

description: Differential cross section, as a function of pseudo-rapidity, from channel (1).
description: DESY-HERA. Differential cross-sections of D*(2010)+- and associated dijet photoproduction in E P collisions at HERA. The variable XOBS(C=GAMMA) is deined as:. (E(jet1)*EXP(-ETARAP(jet1)) + E(jet2)*EXP(-ETARAP(jet2)))/(2*Y*E_e). and is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: and Y = E_gamma/E_e. Decay Channel (1) is D*+ --& gt; D0 PI+s --& gt; (K- PI+) PI+s and CC. Decay Channel (2) is D*+ --& gt; D0 PI+ --& gt; (K- PI+ PI+ PI-) PI+s and CC.
DOI: 10.17182/hepdata.44219.v1/t4
title: "Table 4" of "Measurement of inclusive D*+- and associated dijet cross sections in photoproduction at HERA."

description: Differential cross section, as a function of pseudo-rapidity, from channel (1).
description: DESY-HERA. Differential cross-sections of D*(2010)+- and associated dijet photoproduction in E P collisions at HERA. The variable XOBS(C=GAMMA) is deined as:. (E(jet1)*EXP(-ETARAP(jet1)) + E(jet2)*EXP(-ETARAP(jet2)))/(2*Y*E_e). and is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: and Y = E_gamma/E_e. Decay Channel (1) is D*+ --& gt; D0 PI+s --& gt; (K- PI+) PI+s and CC. Decay Channel (2) is D*+ --& gt; D0 PI+ --& gt; (K- PI+ PI+ PI-) PI+s and CC.
DOI: 10.17182/hepdata.44219.v1/t5
title: "Table 5" of "Measurement of inclusive D*+- and associated dijet cross sections in photoproduction at HERA."

description: Differential cross section for two jet production with associated D* production, from channel (1). The quoted cross sections correspond to the centres of the bins. The second systematic error is that associated with the energy scale.
description: DESY-HERA. Differential cross-sections of D*(2010)+- and associated dijet photoproduction in E P collisions at HERA. The variable XOBS(C=GAMMA) is deined as:. (E(jet1)*EXP(-ETARAP(jet1)) + E(jet2)*EXP(-ETARAP(jet2)))/(2*Y*E_e). and is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: and Y = E_gamma/E_e. Decay Channel (1) is D*+ --& gt; D0 PI+s --& gt; (K- PI+) PI+s and CC. Decay Channel (2) is D*+ --& gt; D0 PI+ --& gt; (K- PI+ PI+ PI-) PI+s and CC.
DOI: 10.17182/hepdata.44219.v1/t6
title: "Table 6" of "Measurement of inclusive D*+- and associated dijet cross sections in photoproduction at HERA."

description: Differential cross section for two jet production with associated D* production, from channel (1). The quoted cross sections correspond to the centres of the bins. The second systematic error is that associated with the energy scale.
description: DESY-HERA. Differential cross-sections of D*(2010)+- and associated dijet photoproduction in E P collisions at HERA. The variable XOBS(C=GAMMA) is deined as:. (E(jet1)*EXP(-ETARAP(jet1)) + E(jet2)*EXP(-ETARAP(jet2)))/(2*Y*E_e). and is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: and Y = E_gamma/E_e. Decay Channel (1) is D*+ --& gt; D0 PI+s --& gt; (K- PI+) PI+s and CC. Decay Channel (2) is D*+ --& gt; D0 PI+ --& gt; (K- PI+ PI+ PI-) PI+s and CC.