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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.
We have measured the inclusive cross-section as a function of missing energy, due to the production of neutrinos or new weakly interacting neutral particles in 450 GeV/c proton-nucleus collisions, using calorimetric measurements of visible event energy. Upper limits are placed on the production of new particles as a function of their energy. These upper limits are typically an order
Differential single diffraction cross section.
Differential single diffraction cross section.
Differential single diffraction cross section.
Slope of experimental fit to differential diffraction cross sections.
Differential single diffraction cross section.
Differential single diffraction cross section.
Differential single diffraction cross section.
Single diffraction cross section parametrized as SIG*MASS**POWER.
Mass dependence of the single diffraction cross section.
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