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Charged particle production has been studied in neutral current deep inelastic ep scattering with the ZEUS detector at HERA using an integrated luminosity of 0.44 fb^-1. Distributions of scaled momenta in the Breit frame are presented for particles in the current fragmentation region. The evolution of these spectra with the photon virtuality, Q^2, is described in the kinematic region 10<Q^2<41000 GeV^2. Next-to-leading-order and modified leading-log-approximation QCD calculations as well as predictions from Monte Carlo models are compared to the data. The results are also compared to e+e- annihilation data. The dependences of the pseudorapidity distribution of the particles on Q^2 and on the energy in the \gamma p system, W, are presented and interpreted in the context of the hypothesis of limiting fragmentation.
Bin averaged scaled momentum spectra in the Q**2 ranges 160 to 320 and 320 to 640 GeV**2.
Bin averaged scaled momentum spectra in the Q**2 ranges 640 to 1280 and 1280 to 2560 GeV**2.
Bin averaged scaled momentum spectra in the Q**2 ranges 2560 to 5120 and 51200 to 10240 GeV**2.
Bin averaged scaled momentum spectra in the Q**2 range 10240 to 20480 GeV**2.
Bin averaged scaled momentum spectra in the Q**2 range 20480 to 40960 GeV**2.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0 to 0.02.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.02 to 0.05.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.05 to 0.1.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.1 to 0.2.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.2 to 0.3.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.3 to 0.4.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.4 to 0.5.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.5 to 0.7.
Number of charged particles per event and per unit of XP as a function of Q**2 in the XP range 0.7 to 1.0.
The normalized charged particle density for the Q**2 range 5120 to 10240 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 2560 to 5120 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 1280 to 2560 GeV in four W ranges.
The normalized charged particle density for the Q**2 range 640 to 1280 GeV in four W ranges.
The normalized charged particle density for the Q**2 range 320 to 640GeV in three W ranges.
The normalized charged particle density for the Q**2 range 160 to 320 GeV in four W ranges.
The normalized charged particle density for the Q**2 range 60 to 160 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 50 to 60 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 40 to 50 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 30 to 40 GeV in three W ranges.
The normalized charged particle density for the Q**2 range 20 to 30 GeV in two W ranges.
The normalized charged particle density for the Q**2 range 10 to 20 GeV in two W ranges.
The reaction gamma p -> p pi0 gamma' has been measured with the Crystal Ball / TAPS detectors using the energy-tagged photon beam at the electron accelerator facility MAMI-B. Energy and angular differential cross sections for the emitted photon gamma' and angular differential cross sections for the pi0 have been determined with high statistics in the energy range of the Delta+(1232) resonance. Cross sections and the ratio of the cross section to the non-radiative process gamma p -> p pi0 are compared to theoretical reaction models, having the anomalous magnetic moment kappa_Delta+ as free parameter. As the shape of the experimental distributions is not reproduced in detail by the model calculations, currently no extraction of kappa_Delta+ is feasible.
Total cross section for the background reaction GAMMA P --> P PI0.
Total cross section for the background reaction GAMMA P --> P PI0 PI0.
Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 at beam energy 400 MeV. Inclusive measurement where only the PI0 decay photons are detected.
Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 at beam energy 400 MeV. Exclusive measurement where only the PI0 decay photons and recoil proton are detected.
Differential cross section as a function of the emitted photon energy for the reaction GAMMA P --> P PI0 GAMMA at beam energy 350 MeV.
Differential cross section as a function of the emitted photon energy for the reaction GAMMA P --> P PI0 GAMMA at beam energy 400 MeV.
Differential cross section as a function of the emitted photon energy for the reaction GAMMA P --> P PI0 GAMMA at beam energy 450 MeV.
Angular distribution of the emitted photon for the reaction GAMMA P --> P PI0 GAMMA at beam energy 350 MeV.
Angular distribution of the emitted photon for the reaction GAMMA P --> P PI0 GAMMA at beam energy 400 MeV.
Angular distribution of the emitted photon for the reaction GAMMA P --> P PI0 GAMMA at beam energy 450 MeV.
Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 GAMMA at beam energy 350 MeV.
Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 GAMMA at beam energy 400 MeV.
Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 GAMMA at beam energy 450 MeV.
Cross section ratio as a function of the emitted photon energy in the reaction GAMMA P --> P PI0 GAMMA for the beam energy 350 MeV.
Cross section ratio as a function of the emitted photon energy in the reaction GAMMA P --> P PI0 GAMMA for the beam energy 400 MeV.
Cross section ratio as a function of the emitted photon energy in the reaction GAMMA P --> P PI0 GAMMA for the beam energy 450 MeV.
Weight averaged total cross sections.
The pseudorapidity density and multiplicity distribution of charged particles produced in proton-proton collisions at the LHC, at a centre-of-mass energy $\sqrt{s} = 7$ TeV, were measured in the central pseudorapidity region |$\eta$| < 1. Comparisons are made with previous measurements at $\sqrt{s}$ = 0.9 TeV and 2.36 TeV. At $\sqrt{s}$ = 7 TeV, for events with at least one charged particle in |$\eta$| < 1, we obtain dNch/deta = 6.01 $\pm$ 0.01 (stat.) $^{+0.20}_{-0.12}$ (syst.). This corresponds to an increase of 57.6% $\pm$ 0.4% (stat.) $^{+3.6}_{-1.8}$% (syst.) relative to collisions at 0.9 TeV, significantly higher than calculations from commonly used models. The multiplicity distribution at 7 TeV is described fairly well by the negative binomial distribution.
Charged-particle pseudorapidity densities at central pseudorapidity (ETRAP from -1.0 to 1.0) for the INEL>0 class of events. Data are also given for the lower energy ALICE data.
Relative increase in pseudorapidity density between the different energies.
Multiplicity distribution normalized to the bin width in the pseudorapidity region -1.0 to 1.0 for INEL>0 collisions at a centre-of-mass energy of 7000 GeV. See the paper arXiv:1004.3034 for the lower energy data. Note that the statistical as well as the systematic uncertainties are strongly correlated between neighbouring points. See text of paper for details.
Pseusdorapidity densities for the INEL>0 class of data as a function of pseudorapidity for centre-of mass energy 0.9 TeV. Note that this data is not in the paper but has been approved by the collaboration.
Pseusdorapidity densities for the INEL>0 class of data as a function of pseudorapidity for centre-of mass energy 2.36 TeV. Note that this data is not in the paper but has been approved by the collaboration.
Pseusdorapidity densities for the INEL>0 class of data as a function of pseudorapidity for centre-of mass energy 7 TeV. Note that this data is not in the paper but has been approved by the collaboration.
The production of leading neutrons, where the neutron carries a large fraction x_L of the incoming proton's longitudinal momentum, is studied in deep-inelastic positron-proton scattering at HERA. The data were taken with the H1 detector in the years 2006 and 2007 and correspond to an integrated luminosity of 122 pb^{-1}. The semi-inclusive cross section is measured in the phase space defined by the photon virtuality 6 < Q^2 < 100 GeV^2, Bjorken scaling variable 1.5x10^{-4} < x < 3x10^{-2}, longitudinal momentum fraction 0.32 < x_L < 0.95 and neutron transverse momentum p_T < 0.2 GeV. The leading neutron structure function, F_2^{LN(3)}(Q^2,x,x_L), and the fraction of deep-inelastic scattering events containing a leading neutron are studied as a function of Q^2, x and x_L. Assuming that the pion exchange mechanism dominates leading neutron production, the data provide constraints on the shape of the pion structure function.
Differential cross section of leading neutron production.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The semi-inclusive leading neutron structure function for Q**2.
The production of prompt photons is measured in the photoproduction regime of electron-proton scattering at HERA. The analysis is based on a data sample corresponding to a total integrated luminosity of 340 pb^-1 collected by the H1 experiment. Cross sections are measured for photons with transverse momentum and pseudorapidity in the range 6 < Et < 15 GeV and -1.0 < eta < 2.4, respectively. Cross sections for events with an additional jet are measured as a function of the transverse energy and pseudorapidity of the jet, and as a function of the fractional momenta x_gamma and x_p carried by the partons entering the hard scattering process. The correlation between the photon and the jet is also studied. The results are compared with QCD predictions based on the collinear and on the k_T factorisation approaches.
Measured inclusive prompt photon cross section in the defined phase space.
Measured prompt photon plus jet cross section in the defined phase space.
Bin averaged differential cross section as a function of ET in the defined phase space.
Bin averaged differential cross section as a function of ET in the defined phase space.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range -1.00 to -0.57.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range -0.57 to 0.20.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 0.20 to 0.94.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 0.94 to 1.42.
Bin averaged double differential cross section for inclusive prompt photon production in bins of ET and the pseudorapidity range 1.42 to 2.43.
Bin averaged differential cross section for prompt photon plus jet as a function of the photon transverse energy.
Bin averaged differential cross section for prompt photon plus jet as a function of the photon pseudorapidity.
Bin averaged differential cross section for prompt photon plus jet as a function of the jet transverse energy.
Bin averaged differential cross section for prompt photon plus jet as a function of the jet pseudorapidity.
Bin averaged differential cross section for prompt photon plus jet as a function of X(C=GAMMA,LO) thelongitudinal momentum fraction of the partons in the photon in LO approximation.
Bin averaged differential cross section for prompt photon plus jet as a function of X(C=P,LO) thelongitudinal momentum fraction of the partons in the proton in LO approximation.
Bin averaged differential cross section for prompt photon plus jet as a function of the photons transverse momentum perpendicular to the jet direction separated into two regions of X(C=GAMMA,LO).
Bin averaged differential cross section for prompt photon plus jet as a function of the difference in azimuthal angle between the photon and the jet separated into two regions of X(C=GAMMA,LO).
We report on double-differential inclusive cross-sections of the production of secondary protons, charged pions, and deuterons, in the interactions with a 5% nuclear interaction length thick stationary carbon target, of proton and pion beams with momentum from \pm 3 GeV/c to \pm 15 GeV/c. Results are given for secondary particles with production angles between 20 and 125 degrees. Cross-sections on carbon nuclei are compared with cross-sections on beryllium, copper, tantalum and lead nuclei.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 20 to 30 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 30 to 45 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 45 to 60 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 65 to 90 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 90 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 degrees.
Beauty production in deep inelastic scattering with events in which a muon and a jet are observed in the final state has been measured with the ZEUS detector at HERA using an integrated luminosity of 114 pb^-1. The fraction of events with beauty quarks in the data was determined using the distribution of the transverse momentum of the muon relative to the jet. The cross section for beauty production was measured in the kinematic range of photon virtuality, Q^2 > 2 Gev^2, and inelasticity, 0.05 < y < 0.7, with the requirement of a muon and a jet. Total and differential cross sections are presented and compared to QCD predictions. The beauty contribution to the structure function F_2 was extracted and is compared to theoretical predictions.
Total visible cross section for BBAR production and decay into MUON+JET.
Measured differential cross section as a function of Q**2.
Measured differential cross section as a function of the muon transverse momentum.
Measured differential cross section as a function of the muon pseudorapidity.
Measured differential cross section as a function of the jet transverse momentum.
Measured differential cross section as a function of the jet pseudorapidity.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 2 to 4 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 4 to 20 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 20 to 45 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 45 to 100 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 100 to 250 GeV**2.
Measured cross sections for beauty production with a muon and jet for the Q**2 bin 250 to 3000 GeV**2.
Extracted values of F2 for B-BBAR production at an X value of 0.00013. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
Extracted values of F2 for B-BBAR production at an X value of 0.0002. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
Extracted values of F2 for B-BBAR production at an X value of 0.0005. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
Extracted values of F2 for B-BBAR production at an X value of 0.002. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
Extracted values of F2 for B-BBAR production at an X value 0.005.
Extracted values of F2 for B-BBAR production at an X value of 0.013. The second systematic error is the uncertainty on the extrapolation to the full muon and jet phase space.
A measurement is presented of inelastic photo- and electroproduction of J/psi mesons in ep scattering at HERA. The data were recorded with the H1 detector in the period from 2004 to 2007. Single and double differential cross sections are determined and the helicity distributions of the J/psi mesons are analysed. The results are compared to theoretical predictions in the colour singlet model and in the framework of non-relativistic QCD. Calculations in the colour singlet model using a k_T factorisation ansatz are able to give a good description of the data, while colour singlet model calculations to next-to-leading order in collinear factorisation underestimate the data.
Measured differential photoproduction cross section as a function of the squared transverse momentum of the J/PSI.
Measured differential photoproduction cross section as a function of the elasticity of the J/PSI.
Measured photoproduction cross section as a function of the photon-proton centre of mass energy W.
Measured differential photoproduction cross sections as a function of the squared transverse momentum of the J/PSI in 4 bins of elasticity.
Measured differential photoproduction cross sections as a function of the elasticity of the J/PSI in 4 bins of transverse momentum.
Measured differential electroproduction cross section as a function of Q**2.
Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P frame.
Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.
Measured differential electroproduction cross section as a function of the photon-proton centre of mass energy W.
Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.
Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.
Measured differential electroproduction cross section as a function of the squared transverse momentum of the J/PSI in the GAMMA* P rest frame.
Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.
Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.
Measured differential electroproduction cross section as a function of the elasticity of the J/PSI.
Measured polarization parameter in the Helicity Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).
Measured polarization parameter in the Collins-Soper Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).
Measured polarization parameter in the Helicity Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).
Measured polarization parameter in the Collins-Soper Frame. Here ALPHA is given by DSIG/DCOS(THETA) ~ 1+ ALPHA COS(THETA)**2 and NU is given by DSIG/DPHI ~ 1+ ALPHA/3 + (NU/3)*COS(2THETA).
We report on double-differential inclusive cross-sections of the production of secondary protons, charged pions, and deuterons, in the interactions with a 5% nuclear interaction length thick stationary lead target, of proton and pion beams with momentum from +/-3 GeV/c to +/-15 GeV/c. Results are given for secondary particles with production angles 20 to 125 degrees. Cross-sections on lead nuclei are compared with cross-sections on beryllium, copper, and tantalum nuclei.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.
Measurements are presented of single and double-differential dijet cross sections in diffractive photoproduction based on a data sample with an integrated luminosity of 47 pb^-1. The events are of the type ep -> eXY, where the hadronic system X contains at least two jets and is separated by a large rapidity gap from the system Y, which consists of a leading proton or low-mass proton excitation. The dijet cross sections are compared with QCD calculations at next-to-leading order and with a Monte Carlo model based on leading order matrix elements with parton showers. The measured cross sections are smaller than those obtained from the next-to-leading order calculations by a factor of about 0.6. This suppression factor has no significant dependence on the fraction x_gamma of the photon four-momentum entering the hard subprocess. Ratios of the diffractive to the inclusive dijet cross sections are measured for the first time and are compared with Monte Carlo models.
Total diffractive dijet positron-proton cross section integrated over the full measured kinematic range.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of X(C=GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of the ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of X(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of Z(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of the absolute difference of the pseudorapidities of the two jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of the dijet invariant mass. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level differential cross section for diffractive dijet production as a function of mass of the diffractive system. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of X(GAMMA) for 3 ranges of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of Z(POMERON) for 2 ranges of X(GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.
Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of X(C=GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.
Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the absolute difference in the pseudorapidities of the 2 jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the invariant mass of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.
Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.
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