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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% {\lambda}int thick stationary aluminium 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 aluminium nuclei are compared with cross-sections on beryllium, carbon, copper, tin, 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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 Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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+ Aluminium interactions at a beam energy of 12.9 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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 Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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+ Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium 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- Aluminium interactions at a beam energy of 15 GeV.
Multiplicity, inclusive, correlation and collective characteristics of multiparticle production processes inK+ Al,K+ Au, π+ Al and π+ Au interactions at 250 GeV/c are studied with the European Hybrid Spectrometer, providing high statistics and almost 4 π acceptance for final state charged particles. It is shown that the proton energy spectrum practically does not depend on the target atomic weight, but the proton angular distributions reveal a strongA-dependence. In a model independent way, the average number of intranuclear collisions is extracted, and it is shown that their dominant part (60% for Al and 80% for Au) is caused by interactions of the non-leading particles produced in the target fragmentation. The multiplication ratio of the produced particles for the Au nucleus changes fromR≃40 at the smallest rapidities in the target fragmentation region, down toR=0.37±0.06 at the largest rapidities in the beam fragmentation region. It is found that the average total longitudinal momentum of the charged products of the beam fragmentation depends weakly on the number of leading hadron (cluster) intranuclear collisions which are characterized by a low inelasticity coefficient 〈k〉=0.17±0.03.
No description provided.
No description provided.
Experimental data are presented on deuteron production in the target fragmentation region for 250 GeV/c π+ interactions with Al and Au nuclei, and compared with analogous data on proton production. Indications are observed for narrow structures in the (dπ-) effective mass system at ∼2.04 and ∼2.08 GeV.
Number of weighted events as a function of number of forward produced deuterons.
Number of weighted events as a function of number of forward produced deuterons.
Mean deuteron multiplicity.
Mean deuteron multiplicity.
Number of weighted events as a function of number of forward produced deuterons.
Number of weighted events as a function of number of forward produced deuterons.
Mean deuteron multiplicity.
Mean deuteron multiplicity.
Number of weighted events as a function of number of forward produced deuterons.
Number of weighted events as a function of number of forward produced deuterons.
Mean deuteron multiplicity.
Mean deuteron multiplicity.
Average deuteron multiplicity as function of the charged particle multiplicity.
Average deuteron multiplicity as function of the charged particle multiplicity.
Average multiplicity of deuterons versus number of produced protons.
Average multiplicity of deuterons versus number of produced protons.
Mean proton multiplicity as a function of charged particle multiplicity.
Mean proton multiplicity as a function of charged particle multiplicity.
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