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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.
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 $\pi^{\pm}$ 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.
Inclusive inelastic scattering spectra from C, Ca, Sn, and Pb were measured for 100-MeV pions at a number of angles. The observed ratios of the π− and π+ total inelastic cross sections for the different targets are explained in terms of a simple model which is based on the assumption that the scattered pion has interacted with only one nucleon. This model also accounts for the ratio between normal and charge-exchange scattering cross sections at 100 MeV.
No description provided.
No description provided.
When you search on a word, e.g. 'collisions', we will automatically search across everything we store about a record. But, sometimes you may wish to be more specific. Here we show you how.
Guidance and examples on the query string syntax can be found in the Elasticsearch documentation.
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