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Measurements of the double-differential proton production cross-section in the range of momentum 0.5 GeV/c < p < 8.0 GeV/c and angle 0.05 rad < \theta < 0.25 rad in collisions of charged pions and protons on beryllium, carbon, aluminium, copper, tin, tantalum and lead are presented. The data were taken with the large acceptance HARP detector in the T9 beam line of the CERN Proton Synchrotron. Incident particles were identified by an elaborate system of beam detectors and impinged on a target of 5 % of a nuclear interaction length. The tracking and identification of the produced particles was performed using the forward spectrometer of the HARP experiment. Results are obtained for the double-differential cross-sections mainly at four incident beam momenta (3 GeV/c, 5 GeV/c, 8 GeV/c and 12 GeV/c). Measurements are compared with predictions of the GEANT4 and MARS Monte Carlo generators.
Differential cross section for proton production with a negative pion beam and Beryllium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Beryllium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Beryllium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Beryllium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Beryllium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Beryllium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Beryllium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Beryllium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Beryllium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Beryllium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Beryllium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Beryllium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Carbon target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Carbon target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Carbon target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Carbon target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Carbon target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Carbon target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Carbon target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Carbon target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Carbon target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Carbon target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Carbon target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Carbon target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Aluminium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Aluminium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Aluminium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Aluminium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Aluminium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Aluminium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Aluminium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Aluminium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Copper target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Copper target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Copper target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Copper target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Copper target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Copper target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Copper target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Copper target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Copper target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Copper target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Copper target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Copper target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Tin target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Tin target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Tin target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Tin target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Tin target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Tin target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Tin target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Tin target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Tin target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Tin target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Tin target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Tin target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Tantallum target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Tantallum target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Tantallum target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Tantallum target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Tantallum target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Tantallum target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Tantallum target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Tantallum target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Tantallum target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Tantallum target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Tantallum target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Tantallum target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Lead target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Lead target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Lead target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a negative pion beam and Lead target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Lead target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Lead target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Lead target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a positive pion beam and Lead target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Lead target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Lead target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Lead target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
Differential cross section for proton production with a proton beam and Lead target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.
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 tantalum 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 between 20 and 125 degrees. They are of particular relevance for the optimization of the design parameters of the proton driver of a neutrino factory.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
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 DEG.
The measured deuteron to proton ratio for the P beam as a function of the momentum at the vertex for the angular range 20 to 30 DEG.
The measured deuteron to proton ratio for the P beam as a function of the momentum at the vertex for the angular range 30 to 45 DEG.
The measured deuteron to proton ratio for the P beam as a function of the momentum at the vertex for the angular range 45 to 65 DEG.
The measured deuteron to proton ratio for the P beam as a function of the momentum at the vertex for the angular range 65 to 90 DEG.
The measured deuteron to proton ratio for the P beam as a function of the momentum at the vertex for the angular range 90 to 125 DEG.
The measured deuteron to proton ratio for the PI- beam as a function of the momentum at the vertex for the angular range 20 to 30 DEG.
The measured deuteron to proton ratio for the PI- beam as a function of the momentum at the vertex for the angular range 30 to 45 DEG.
The measured deuteron to proton ratio for the PI- beam as a function of the momentum at the vertex for the angular range 45 to 65 DEG.
The measured deuteron to proton ratio for the PI- beam as a function of the momentum at the vertex for the angular range 65 to 90 DEG.
The measured deuteron to proton ratio for the PI- beam as a function of the momentum at the vertex for the angular range 90 to 125 DEG.
The measured deuteron to proton ratio for the PI+ beam as a function of the momentum at the vertex for the angular range 20 to 30 DEG.
The measured deuteron to proton ratio for the PI+ beam as a function of the momentum at the vertex for the angular range 30 to 45 DEG.
The measured deuteron to proton ratio for the PI+ beam as a function of the momentum at the vertex for the angular range 45 to 65 DEG.
The measured deuteron to proton ratio for the PI+ beam as a function of the momentum at the vertex for the angular range 65 to 90 DEG.
The measured deuteron to proton ratio for the PI+ beam as a function of the momentum at the vertex for the angular range 90 to 125 DEG.
The collisions ofp,2H,4He and C with carbon and tantalum nuclei at 4.2 GeV/c per nucleon as well as the collisionsp-C andp-Ta at 10 GeV/c from 2-m propane bubble chamber have been studied. New results on nuclear stopping have been obtained from the examination of proton rapidity distributions and average rapidity of leading protons for collisions of various degree of centrality: our study points out that a proton projectile is fully stopped in the centralp-Ta collisions at 4.2 GeV/c but only partly stopped at 10 Gev/c. The proton multiplicity in the centralp-Ta collisions at 10 GeV/c can be described by the binomial distribution,P(n), which expresses the probability that the projectile meetsn protons among the nucleons being along the diameter of a target nucleus.
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