Showing 4 of 4 results
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.
Measurements of the double-differential charged pion production cross-section in the range of momentum 0.5 GeV/c < p < 8.0 GeV/c and angle 0.025 rad < theta <0.25 rad in collisions of protons on beryllium, carbon, nitrogen, oxygen, 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 PS. Incident particles were identified by an elaborate system of beam detectors. The data were taken with thin targets of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using the forward system of the HARP experiment. Results are obtained for the double-differential cross section mainly at four incident proton beam momenta (3 GeV/c, 5 GeV/c, 8 GeV/c and 12 GeV/c). Measurements are compared with the GEANT4 and MARS Monte Carlo generators. A global parametrization is provided as an approximation of all the collected datasets which can serve as a tool for quick yields estimates.
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We report on double-differential inclusive cross-sections of the production of secondary protons and charged pions, in the interactions with a 5% interaction length thick stationary beryllium 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.
Double differential inclusive cross section for the reaction P BE --> P X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 3 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 3 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 3 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 3 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 3 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 3 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 3 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 3 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 5 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 5 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 5 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 5 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 5 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 5 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 5 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 5 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 12 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 12 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 12 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 12 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 12 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 12 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 12 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 12 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with a 15 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ X with a 15 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- X with a 15 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P X with a 15 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with a 15 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with a 15 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P X with a 15 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with a 15 GeV beam and production angles 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 15 GeV beam and production angles 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 15 GeV beam and production angles 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 15 GeV beam and production angles 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 15 GeV beam and production angles 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 15 GeV beam and production angles 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 15 GeV beam and production angles 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 15 GeV beam and production angles 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with a 15 GeV beam and production angles 105 to 125 degrees.
An analysis of inclusive pion production in proton-beryllium collisions at 6.4, 12.3, and 17.5 GeV/c proton beam momentum has been performed. The data were taken by Experiment 910 at the Alternating Gradient Synchrotron at the Brookhaven National Laboratory. The differential $\pi^+$ and $\pi^-$ production cross sections ($d^2\sigma/dpd\Omega$) are measured up to 400 mRad in $\theta_{\pi}$ and up to 6 GeV/c in $p_{\pi}$. The measured cross section is fit with a Sanford-Wang parameterization.
Pion production cross section for 6.4 GeV incident protons.
Pion production cross section for 6.4 GeV incident protons.
Pion production cross section for 6.4 GeV incident protons.
Pion production cross section for 6.4 GeV incident protons.
Pion production cross section for 12.3 GeV incident protons.
Pion production cross section for 12.3 GeV incident protons.
Pion production cross section for 12.3 GeV incident protons.
Pion production cross section for 12.3 GeV incident protons.
Pion production cross section for 12.3 GeV incident protons.
Pion production cross section for 12.3 GeV incident protons.
Pion production cross section for 17.5 GeV incident protons.
Pion production cross section for 17.5 GeV incident protons.
Pion production cross section for 17.5 GeV incident protons.
Pion production cross section for 17.5 GeV incident protons.
Pion production cross section for 17.5 GeV incident protons.
Pion production cross section for 17.5 GeV incident protons.
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