Showing 6 of 6 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.
We report on double-differential inclusive cross-sections of the production of secondary protons, deuterons, and charged pions and kaons, in the interactions with a 5% nuclear interaction length thick stationary beryllium target, of a +8.9 GeV/c proton and pion beam, and a -8.0 GeV/c pion beam. 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 an 8.9 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 105 to 125 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 105 to 125 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 20 to 30 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 30 to 40 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 40 to 50 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 50 to 60 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 60 to 75 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 75 to 90 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 90 to 105 degrees.
Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 105 to 125 degrees.
Ratio K+/PI+ in 8.9 GeV proton and PI+ interactions with Beryllium.
Ratio of deuteron to proton production in P BE interactions at 8.9 GeV.
Ratio of deuteron to proton production in PI+ BE interactions at 8.9 GeV.
Ratio of deuteron to proton production in PI- BE interactions at 8.0 GeV.
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.
This paper presents the results on charged particle yields and production ratios as measured by the NA56/SPY experiment for 450 GeV/c proton interactions on beryllium targets. The data cover a seconda
Positive particle yield from the 100mm Be target. Data are corrected for the pion or proton flux coming from strange particle decays.
Negative particle yield from the 100mm Be target. Data are corrected for the pion or antiproton flux coming from strange particle decays.
Positive particle yield from the 100mm Be target. Data are NOT corrected for the pion or proton flux coming from strange particle decays.
Negative particle yield from the 100mm Be target. Data are NOT corrected for the pion or antiproton flux coming from strange particle decays.
Ratio of kaon to pion production with the 100mm Be target. Data are corrected for the pion flux from strange particle decays.
Ratio of kaon to pion production with the 100mm Be target. Data are NOT corrected for the pion flux from strange particle decays.
Ratio of kaon to proton or antiproton production with the 100mm Be target. Data are corrected for the proton or antiproton flux from strange particle decays.
Ratio of kaon to proton or antiproton production with the 100mm Be target. Data are NOT corrected for the proton or antiproton flux from strange particle decays.
Ratio of pion to proton or antiproton production with the 100mm Be target. Data are corrected for the pion, proton or antiproton flux from strange particledecays.
Ratio of pion to proton or antiproton production with the 100mm Be target. Data are NOT corrected for the pion, proton or antiproton flux from strange particle decays.
Positive pion yields with the 100mm Be target as a function of transverse momentum. Data are corrected for the pion flux coming from strange particle decays. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Negative pion yields with the 100mm Be target as a function of transverse momentum. Data are corrected for the pion flux coming from strange particle decays. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Positive pion yields with the 100mm Be target as a function of transverse momentum. Data are NOT corrected for the pion flux coming from strange particle decays. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Negative pion yields with the 100mm Be target as a function of transverse momentum. Data are NOT corrected for the pion flux coming from strange particle decays. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Positive kaon yields with the 100mm Be target as a function of transverse momentum. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Negative kaon yields with the 100mm Be target as a function of transverse momentum. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Proton yields with the 100mm Be target as a function of transverse momentum. Data are corrected for the proton flux coming from strange particle decays. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Antiproton yields with the 100mm Be target as a function of transverse momentum. Data are corrected for the antiproton flux coming from strange particle decays. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Proton yields with the 100mm Be target as a function of transverse momentum. Data are NOT corrected for the proton flux coming from strange particle decays. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Antiproton yields with the 100mm Be target as a function of transverse momentum. Data are NOT corrected for the antiproton flux coming from strange particle decays. Additional systematic error of 10 PCT (5 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of positive kaon to pion yields with the 100mm Be target as a function of the transverse momentum. Data are corrected for the pion flux coming from strange particle decays. Additional systematic error of 1.3 PCT (1.1 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of negative kaon to pion yields with the 100mm Be target as a function of the transverse momentum. Data are corrected for the pion flux coming from strange particle decays. Additional systematic error of 1.3 PCT (1.1 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of positive kaon to pion yields with the 100mm Be target as a function of the transverse momentum. Data are NOT corrected for the pion flux coming from strange particle decays. Additional systematic error of 1.3 PCT (1.1 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of negative kaon to pion yields with the 100mm Be target as a function of the transverse momentum. Data are NOT corrected for the pion flux coming from strange particle decays. Additional systematic error of 1.3 PCT (1.1 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of the positive kaon to proton yields with the 100mm Be target as a function of the transverse momentum. Data are corrected for the proton flux coming from strange particle decays. Additional systematic error of 1.7 PCT (1.5 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of the negative kaon to antiproton yields with the 100mm Be target asa function of the transverse momentum. Data are corrected for the antiproton fl ux coming from strange particle decays. Additional systematic error of 1.7 PCT (1.5 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of the positive kaon to proton yields with the 100mm Be target as a function of the transverse momentum. Data are NOT corrected for the proton flux coming from strange particle decays. Additional systematic error of 1.7 PCT (1.5 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of the negative kaon to antiproton yields with the 100mm Be target asa function of the transverse momentum. Data are NOT corrected for the antiproto n flux coming from strange particle decays. Additional systematic error of 1.7 PCT (1.5 PCT) at PLAB = 15 GeV (40 GeV).
Ratio of the proton to positive pion yields with the 100mm Be target as a function of the transverse momentum. Data are corrected for the pion and proton flux coming from strange particle decays. Additional systematic error of 1.1 PCT.
Ratio of the antiproton to negative pion yields with the 100mm Be target asa function of the transverse momentum. Data are corrected for the pion and anti proton flux coming from strange particle decays. Additional systematic error of 1.1 PCT.
Ratio of the proton to positive pion yields with the 100mm Be target as a function of the transverse momentum. Data are NOT corrected for the pion and proton flux coming from strange particle decays. Additional systematic error of 1.1 PCT.
Ratio of the antiproton to negative pion yields with the 100mm Be target asa function of the transverse momentum. Data are NOT corrected for the pion and antiproton flux coming from strange particle decays. Additional systematic error of 1.1 PCT.
Yields from a 200mm Be target relative to the 100mm Be target. The quoted error includes statistical and systematic uncertainties.
Yields from a 300mm Be target relative to the 100mm Be target. The quoted error includes statistical and systematic uncertainties.
We have measured the inclusive cross-section as a function of missing energy, due to the production of neutrinos or new weakly interacting neutral particles in 450 GeV/c proton-nucleus collisions, using calorimetric measurements of visible event energy. Upper limits are placed on the production of new particles as a function of their energy. These upper limits are typically an order
Differential single diffraction cross section.
Differential single diffraction cross section.
Differential single diffraction cross section.
Slope of experimental fit to differential diffraction cross sections.
Differential single diffraction cross section.
Differential single diffraction cross section.
Differential single diffraction cross section.
Single diffraction cross section parametrized as SIG*MASS**POWER.
Mass dependence of the single diffraction cross section.
None
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
When you search on a word, e.g. 'collisions', we will automatically search across everything we store about a record. But sometimes you may wish to be more specific. Here we show you how.
Guidance on the query string syntax can also be found in the OpenSearch documentation.
About HEPData Submitting to HEPData HEPData File Formats HEPData Coordinators HEPData Terms of Use HEPData Cookie Policy
Status Email Forum Twitter GitHub
Copyright ~1975-Present, HEPData | Powered by Invenio, funded by STFC, hosted and originally developed at CERN, supported and further developed at IPPP Durham.