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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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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 tin target, of proton and pion beams with momentum from \pm3 GeV/c to \pm15 GeV/c. Results are given for secondary particles with production angles between 20 and 125 degrees. Cross-sections on tin nuclei are compared with cross-sections on beryllium, carbon, copper, tantalum and lead nuclei.
Ratio of deuterons to protons for polar angle 20-30 deg.
Ratio of deuterons to protons for polar angle 30-45 deg.
Ratio of deuterons to protons for polar angle 45-65 deg.
Ratio of deuterons to protons for polar angle 65-90 deg.
Ratio of deuterons to protons for polar angle 90-125 deg.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
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