Showing 10 of 14 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, charged pions, and deuterons, in the interactions with a 5% nuclear interaction length thick stationary lead target, of proton and pion beams with momentum from +/-3 GeV/c to +/-15 GeV/c. Results are given for secondary particles with production angles 20 to 125 degrees. Cross-sections on lead nuclei are compared with cross-sections on beryllium, copper, and tantalum nuclei.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.
Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.
Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.
Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.
Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.
The HARP collaboration has presented measurements of the double-differential pi+/pi- production cross-section in the range of momentum 100 MeV/c <= p 800 MeV/c and angle 0.35 rad <= theta <= 2.15 rad with proton beams hitting thin nuclear targets. In many applications the extrapolation to long targets is necessary. In this paper the analysis of data taken with long (one interaction length) solid cylindrical targets made of carbon, tantalum and lead is presented. The data were taken with the large acceptance HARP detector in the T9 beam line of the CERN PS. The secondary pions were produced by beams of protons with momenta 5 GeV/c, 8 GeV/c and 12 GeV/c. The tracking and identification of the produced particles were performed using a small-radius cylindrical time projection chamber (TPC) placed inside a solenoidal magnet. Incident protons were identified by an elaborate system of beam detectors. Results are obtained for the double-differential yields per target nucleon d2 sigma / dp dtheta. The measurements are compared with predictions of the MARS and GEANT4 Monte Carlo simulations.
Differential cross section for PI+ production with a C target in the angular range 0.35 to 0.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a C target in the angular range 0.55 to 0.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a C target in the angular range 0.75 to 0.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a C target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a C target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a C target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a C target in the angular range 1.55 to 1.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a C target in the angular range 1.75 to 1.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a C target in the angular range 1.95 to 2.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 0.35 to 0.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 0.55 to 0.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 0.75 to 0.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 1.55 to 1.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 1.75 to 1.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a C target in the angular range 1.95 to 2.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 0.35 to 0.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 0.55 to 0.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 0.75 to 0.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 1.55 to 1.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 1.75 to 1.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a TA target in the angular range 1.95 to 2.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 0.35 to 0.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 0.55 to 0.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 0.75 to 0.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 1.55 to 1.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 1.75 to 1.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a TA target in the angular range 1.95 to 2.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 0.35 to 0.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 0.55 to 0.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 0.75 to 0.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 1.55 to 1.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 1.75 to 1.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI+ production with a PB target in the angular range 1.95 to 2.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 0.35 to 0.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 0.55 to 0.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 0.75 to 0.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 1.55 to 1.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 1.75 to 1.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Differential cross section for PI- production with a PB target in the angular range 1.95 to 2.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
Measurements of the double-differential pi+/- production cross-section in the range of momentum 100 MeV/c <= p <= 800 MeV/c and angle 0.35 rad <= theta <= 2.15 rad using pi+/- beams incident on beryllium, aluminium, carbon, copper, tin, tantalum and lead targets are presented. The data were taken with the large acceptance HARP detector in the T9 beam line of the CERN PS. The secondary pions were produced by beams in a momentum range from 3 GeV/c to 12.9 GeV/c hitting a solid target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using a small-radius cylindrical time projection chamber (TPC) placed inside a solenoidal magnet. Incident particles were identified by an elaborate system of beam detectors. Results are obtained for the double-differential cross-sections d2sigma/dpdtheta at six incident beam momenta. Data at 3 GeV/c, 5 GeV/c, 8 GeV/c, and 12 GeV/c are available for all targets while additional data at 8.9 GeV/c and 12.9 GeV/c were taken in positive particle beams on Be and Al targets, respectively. The measurements are compared with several generators of GEANT4 and the MARS Monte Carlo simulation.
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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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Measurements of the double-differential $\pi^{\pm}$ production cross-section in the range of momentum $0.5 \GeVc \leq p \le 8.0 \GeVc$ and angle $0.025 \rad \leq \theta \le 0.25 \rad$ in interactions of charged pions on beryllium, carbon, aluminium, copper, tin, tantalum and lead are presented. These data represent the first experimental campaign to systematically measure forward pion hadroproduction. The data were taken with the large acceptance HARP detector in the T9 beam line of the CERN PS. Incident particles, impinging on a 5% nuclear interaction length target, were identified by an elaborate system of beam detectors. The tracking and identification of the produced particles was performed using the forward spectrometer of the HARP detector. Results are obtained for the double-differential cross-sections $ {{\mathrm{d}^2 \sigma}}/{{\mathrm{d}p\mathrm{d}\Omega}} $ mainly at four incident pion beam momenta (3 \GeVc, 5 \GeVc, 8 \GeVc and 12 \GeVc). The measurements are compared with the GEANT4 and MARS Monte Carlo simulation
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 3, 5, 8, and 12 GeV for the angular range 0.050 to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 3, 5, 8, and 12 GeV for the angular range 0.100 to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 3, 5, 8, and 12 GeV for the angular range 0.150 to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 3, 5, 8, and 12 GeV for the angular range 0.200 to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 3, 5, 8, and 12 GeV for the angular range 0.050 to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 3, 5, 8, and 12 GeV for the angular range 0.100 to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 3, 5, 8, and 12 GeV for the angular range 0.150 to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 3, 5, 8, and 12 GeV for the angular range 0.200 to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 8 and 12 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 8 and 12 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- BE interactions at 8 and 12 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 8 and 8.9 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 8 and 8.9 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ BE interactions at 8 and 8.9 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 3, 5, 8 GeV for the angular range 0.050 to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 3, 5, 8 GeV for the angular range 0.100 to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 3, 5, 8 GeV for the angular range 0.150 to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 3, 5, 8 GeV for the angular range 0.200 to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 3, 5, 8 GeV for the angular range 0.050 to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 3, 5, 8 GeV for the angular range 0.100 to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 3, 5, 8 GeV for the angular range 0.150 to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 3, 5, 8 GeV for the angular range 0.200 to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 8 and 12 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 8 and 12 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- C interactions at 8 and 12 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 8 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 8 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ C interactions at 8 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.050to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.100to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.150to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.200to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.050to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.100to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.150to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 3, 5, 8 and 12 GeV for the angular range 0.200to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 8 and 12 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 8 and 12 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- AL interactions at 8 and 12 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 8 and 12.9 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 8 and 12.9 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ AL interactions at 8 and 12.9 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.050to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.100to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.150to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.200to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.050to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.100to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.150to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 3, 5, 8 and 12 GeV for the angular range 0.200to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 8 and 12 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 8 and 12 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- CU interactions at 8 and 12 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 8 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 8 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ CU interactions at 8 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.050to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.100to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.150to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.200to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.050to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.100to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.150to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 3, 5, 8 and 12 GeV for the angular range 0.200to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 8 and 12 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 8 and 12 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- SN interactions at 8 and 12 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 8 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 8 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ SN interactions at 8 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.050to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.100to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.150to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.200to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.050to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.100to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.150to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 3, 5, 8 and 12 GeV for the angular range 0.200to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 8 and 12 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 8 and 12 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- TA interactions at 8 and 12 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 8 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 8 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ TA interactions at 8 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 3, 5, 8 and 12 GeV for the angular range 0.05 to 0.10 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 3, 5, 8 and 12 GeV for the angular range 0.10 to 0.15 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 3, 5, 8 and 12 GeV for the angular range 0.15 to 0.20 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 3, 5, 8 and 12 GeV for the angular range 0.20 to 0.25 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 3, 5, 8 ans 112 GeV for the angular range 0.050 to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 3, 5, 8 ans 112 GeV for the angular range 0.100 to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 3, 5, 8 ans 112 GeV for the angular range 0.150 to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 3, 5, 8 ans 112 GeV for the angular range 0.200 to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 3, 5, 8 ans 112 GeV for the angular range 0.050 to 0.100 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 3, 5, 8 ans 112 GeV for the angular range 0.100 to 0.150 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 3, 5, 8 ans 112 GeV for the angular range 0.150 to 0.200 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 3, 5, 8 ans 112 GeV for the angular range 0.200 to 0.250 radians.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 8 and 12 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 8 and 12 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI- PB interactions at 8 and 12 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 8 GeV for the angular range 0.025 to 0.050 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 8 GeV for the angular range 0.050 to 0.075 radians with finer binning.
Double differential PI+ and PI- production cross section in the laboratory system for PI+ PB interactions at 8 GeV for the angular range 0.075 to 0.100 radians with finer binning.
Measurements of the double-differential charged pion production cross-section in the range of momentum 100 MeV/c < p < 800 MeV/c and angle 0.35 < \theta < 2.15 rad in proton-beryllium, proton-carbon, proton-aluminium, proton-copper, proton-tin, proton-tantalum and proton-lead collisions are presented. The data were taken with the large acceptance HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 GeV/c to 12.9 GeV/c hitting a target with a thickness of 5% of a nuclear interaction length.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.95 to 2.15 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.95 to 2.15 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the AL target for a PI+ polar angle from 0.35 to 0.55 radians.
The results of the measurements of the double-differential production cross-sections of pions in p-C and $\pi^\pm$-C interactions using the forward spectrometer of the HARP experiment are presented. The incident particles are 12 GeV/c protons and charged pions directed onto a carbon target with a thickness of 5% of a nuclear interaction length. For p-C interactions the analysis is performed using 100035 reconstructed secondary tracks, while the corresponding numbers of tracks for $\pi^-$-C and $\pi^+$-C analyses are 106534 and 10122 respectively. Cross-section results are presented in the kinematic range 0.5 GeV/c $\leq p_{\pi} <$ 8 GeV/c and 30 mrad $\leq \theta_{\pi} <$ 240 mrad in the laboratory frame. The measured cross-sections have a direct impact on the precise calculation of atmospheric neutrino fluxes and on the improved reliability of extensive air shower simulations by reducing the uncertainties of hadronic interaction models in the low energy range.
Double-differential cross section for 12 GeV proton-carbon interactions with the scattered polar angle 30 to 60 mrad.
Double-differential cross section for 12 GeV proton-carbon interactions with the scattered polar angle 60 to 90 mrad.
Double-differential cross section for 12 GeV proton-carbon interactions with the scattered polar angle 90 to 120 mrad.
Double-differential cross section for 12 GeV proton-carbon interactions with the scattered polar angle 120 to 150 mrad.
Double-differential cross section for 12 GeV proton-carbon interactions with the scattered polar angle 150 to 180 mrad.
Double-differential cross section for 12 GeV proton-carbon interactions with the scattered polar angle 180 to 210 mrad.
Double-differential cross section for 12 GeV proton-carbon interactions with the scattered polar angle 210 to 240 mrad.
Double-differential cross section for 12 GeV positive pion-carbon interactions with the scattered polar angle 30 to 60 mrad.
Double-differential cross section for 12 GeV positive pion-carbon interactions with the scattered polar angle 60 to 90 mrad.
Double-differential cross section for 12 GeV positive pion-carbon interactions with the scattered polar angle 90 to 120 mrad.
Double-differential cross section for 12 GeV positive pion-carbon interactions with the scattered polar angle 120 to 150 mrad.
Double-differential cross section for 12 GeV positive pion-carbon interactions with the scattered polar angle 150 to 180 mrad.
Double-differential cross section for 12 GeV positive pion-carbon interactions with the scattered polar angle 180 to 210 mrad.
Double-differential cross section for 12 GeV negative pion-carbon interactions with the scattered polar angle 30 to 60 mrad.
Double-differential cross section for 12 GeV negative pion-carbon interactions with the scattered polar angle 60 to 90 mrad.
Double-differential cross section for 12 GeV negative pion-carbon interactions with the scattered polar angle 90 to 120 mrad.
Double-differential cross section for 12 GeV negative pion-carbon interactions with the scattered polar angle 120 to 150 mrad.
Double-differential cross section for 12 GeV negative pion-carbon interactions with the scattered polar angle 150 to 180 mrad.
Double-differential cross section for 12 GeV negative pion-carbon interactions with the scattered polar angle 180 to 210 mrad.
Measurements of double-differential charged pion production cross-sections in interactions of 12 GeV/c protons on O_2 and N_2 thin targets are presented in the kinematic range 0.5 GeV/c < p_{\pi} < 8 GeV/c and 50 mrad < \theta_{\pi} < 250 mrad (in the laboratory frame) and are compared with p--C results. For p--N_2 (p--O_2) interactions the analysis is performed using 38576 (7522) reconstructed secondary pions. The analysis uses the beam instrumentation and the forward spectrometer of the HARP experiment at CERN PS. The measured cross-sections have a direct impact on the precise calculation of atmospheric neutrino fluxes and on the improved reliability of extensive air shower simulations by reducing the uncertainties of hadronic interaction models in the low energy range. In particular, the present results allow the common hypothesis that p--C data can be used to predict the p--N_2 and p--O_2 pion production cross-sections to be tested.
Double differential cross section for pion production in P-N2 interactions for the pion scattered polar angle range 50 to 100 mrad.
Double differential cross section for pion production in P-N2 interactions for the pion scattered polar angle range 100 to 150 mrad.
Double differential cross section for pion production in P-N2 interactions for the pion scattered polar angle range 150 to 200 mrad.
Double differential cross section for pion production in P-N2 interactions for the pion scattered polar angle range 200 to 250 mrad.
Double differential cross section for pion production in P-O2 interactions for the pion scattered polar angle range 50 to 100 mrad.
Double differential cross section for pion production in P-O2 interactions for the pion scattered polar angle range 100 to 150 mrad.
Double differential cross section for pion production in P-O2 interactions for the pion scattered polar angle range 150 to 200 mrad.
Double differential cross section for pion production in P-O2 interactions for the pion scattered polar angle range 200 to 250 mrad.
Double differential cross section for pion production in P-C2 interactions for the pion scattered polar angle range 50 to 100 mrad.. The data have been previously published (ASTROPHYS 29,257(2008)) but are presented here with different binning for comparison with the O and N data.
Double differential cross section for pion production in P-C2 interactions for the pion scattered polar angle range 100 to 150 mrad.. The data have been previously published (ASTROPHYS 29,257(2008)) but are presented here with different binning for comparison with the O and N data.
Double differential cross section for pion production in P-C2 interactions for the pion scattered polar angle range 150 to 200 mrad.. The data have been previously published (ASTROPHYS 29,257(2008)) but are presented here with different binning for comparison with the O and N data.
Double differential cross section for pion production in P-C2 interactions for the pion scattered polar angle range 200 to 250 mrad.. The data have been previously published (ASTROPHYS 29,257(2008)) but are presented here with different binning for comparison with the O and N data.
A measurement of the double-differential $\pi^{\pm}$ production cross-section in proton--carbon, proton--copper and proton--tin collisions in the range of pion momentum $100 \MeVc \leq p < 800 \MeVc$ and angle $0.35 \rad \le \theta <2.15 \rad$ is presented. The data were taken with the HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 \GeVc to 12 \GeVc hitting a target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was done using a small-radius cylindrical time projection chamber (TPC) placed in a solenoidal magnet. An elaborate system of detectors in the beam line ensured the identification of the incident particles. Results are shown for the double-differential cross-sections at four incident proton beam momenta (3 \GeVc, 5 \GeVc, 8 \GeVc and 12 \GeVc).
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI+ production from C in the LAB system for PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI- production from C in the LAB system for PI- polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI+ production from CU in the LAB system for PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI- production from CU in the LAB system for PI- polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI+ production from SN in the LAB system for PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI- production from SN in the LAB system for PI- polar angle from 1.95 to 2.15 radians.
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