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Particle production in proton-induced reactions at 14.6 GeV/c on Be, Al, Cu, and Au targets has been systematically studied using the E-802 spectrometer at the BNL-Alternating Gradient Synchrotron. Particles are measured in the angular range from 5° to 58° and identified up to momenta of 5, 3.5, and 8 GeV/c for pions, kaons, and protons, respectively. Mechanisms for particle production are discussed in comparison with heavy-ion-induced reactions at the same incident energy per nucleon.
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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 copper 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.
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 ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 20 to 30 DEG.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 30 to 45 DEG.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 45 to 65 DEG.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 65 to 90 DEG.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 90 to 125 DEG.
Highly inelastic processes in hadron-nucleus reactions at several GeV have been studied by measuring multi-particle emission in the target-rapidity region. Events with no leading particle(s) but with high multiplicities were observed up to 4 GeV. Proton spectra from such events were well reproduced with a single-moving-source model, which implied possible formation of a local source. The number of nucleons involved in the source was estimated to be (3–5)A 1 3 from the source velocity and the multiplicity of emitted protons. In those processes the incident energy flux seemed to be deposited totally or mostly (>62;75%) in the target nucleus to form the local source. The cross sections for the process were about 30% of the geometrical cross sections, with little dependence on incident energies up to 4 GeV and no dependence on projectiles (pions or protons). The E 0 parameter in the invariant-cross-section formula E d 3 σ /d p 3 = A exp (− E / E 0 ) for protons from the source increases with incident energy from 1 to 4 GeV/ c , but seems to saturate above 10 GeV at a value E 0 = 60–70 MeV. Three components in the emitted nucleon spectra were observed which would correspond to three stages of the reaction process: primary, pre-equilibrium and equilibrium.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
BEAM ERROR D(P)/P = 0.300 PCT. X ERROR D(EKIN)/EKIN = 8.00 PCT.
Inclusive cross sections for production of π+, π−, p, d, H3, He3, and He4 have been measured at laboratory angles from 10° to 145° in nuclear collisions of Ne + Naf, Ne + Cu, and Ne + Pb at 400 MeV/nucleon, C + C, C + Pb, Ne + NaF, Ne + Cu, Ne + Pb, Ar + KCl, and Ar + Pb at 800 MeV/nucleon, and Ne + NaF and Ne + Pb at 2.1 GeV/nucleon. The production of light fragments in proton induced collisions at beam energies of 800 MeV and 2.1 GeV has also been measured in order to allow us to compare these processes. For equal-mass nuclear collisions the total integrated yields of nuclear charges are well explained by a simple participant-spectator model. For 800 MeV/nucleon beams the energy spectra of protons at c.m. 90° are characterized by a "shoulder-arm" type of spectrum shape with an exponential falloff at high energies, whereas those of pions are of a simple exponential type. The inverse of the exponential slope, E0, for protons is systematically larger than that for pions. This value of E0 is larger for heavier-mass projectiles and targets. It also increases monotonically with the beam energy. The angular anisotropy of protons is larger than that of pions. The yield ratio of π− to total nuclear charge goes up with the beam energy, whereas the yields of composite fragments decrease. The ratio of low-energy π− to π+, as well as that of H3 to He3, is larger than the neutron to proton ratio of the system. The spectrum shape of the composite fragments with mass number A is explained very well by the Ath power of the observed proton spectra. The sizes of the interaction region are evaluated from the observed coalescence coefficients. The radius obtained is typically 3-4 fm. The yield ratio of composite fragments to protons strongly depends on the projectile and target masses and the beam energy, but not on the emission angle of the fragments. These results are compared with currently available theoretical models. NUCLEAR REACTIONS Ne + NaF, Ne + Cu, Ne + Pb, EA=400 MeV/nucleon; C + C, C + Pb, Ne + NaF, Ne + Cu, Ne + Pb, Ar + KCl, Ar + Pb, EA=800 MeV/nucleon; Ne + NaF, Ne + Pb, EA=2100 MeV/nucleon; p + C, p+ NaF, p + KCl, p + Cu, p + Pb, E=800 MeV; p + C, p + NaF, p + KCl, p + Cu, p + Pb, E=2100 MeV; measured σ(p,θ) for π+, π−, p, d, H3, He3, and He4.
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