Showing 6 of 6 results
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.
Measurements of the double-differential charged pion production cross-section in the range of momentum 0.5 GeV/c < p < 8.0 GeV/c and angle 0.025 rad < theta <0.25 rad in collisions of protons on beryllium, carbon, nitrogen, oxygen, aluminium, copper, tin, tantalum and lead are presented. The data were taken with the large acceptance HARP detector in the T9 beam line of the CERN PS. Incident particles were identified by an elaborate system of beam detectors. The data were taken with thin targets of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using the forward system of the HARP experiment. Results are obtained for the double-differential cross section mainly at four incident proton beam momenta (3 GeV/c, 5 GeV/c, 8 GeV/c and 12 GeV/c). Measurements are compared with the GEANT4 and MARS Monte Carlo generators. A global parametrization is provided as an approximation of all the collected datasets which can serve as a tool for quick yields estimates.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
Measurements of the double-differential charged pion production cross-section in the range of momentum 100 MeV/c < p < 800 MeV/c and angle 0.35 < \theta < 2.15 rad in proton-beryllium, proton-carbon, proton-aluminium, proton-copper, proton-tin, proton-tantalum and proton-lead collisions are presented. The data were taken with the large acceptance HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 GeV/c to 12.9 GeV/c hitting a target with a thickness of 5% of a nuclear interaction length.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the BE target for a PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the BE target for a PI- polar angle from 1.95 to 2.15 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the C target for a PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for inclusive PI- production in the LAB system with the C target for a PI- polar angle from 1.95 to 2.15 radians.
Double-differential cross section for inclusive PI+ production in the LAB system with the AL target for a PI+ polar angle from 0.35 to 0.55 radians.
Measurements of the double-differential $\pi^{\pm}$ production cross-section in the range of momentum $100 \MeVc \leq p < 800 \MeVc$ and angle $0.35 \rad \leq \theta < 2.15 \rad$ in proton--beryllium, proton--aluminium and proton--lead collisions are presented. The data were taken with the HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 \GeVc to 12.9 \GeVc hitting a target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using a small-radius cylindrical time projection chamber (TPC) placed inside a solenoidal magnet. Incident particles were identified by an elaborate system of beam detectors. Results are obtained for the double-differential cross-sections at six incident proton beam momenta (3 \GeVc, 5 \GeVc, 8 \GeVc, 8.9 \GeVc (Be only), 12 \GeVc and 12.9 \GeVc (Al only)) and compared to previously available data.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI- production from BE in the LAB system for PI- polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI+ production from AL in the LAB system for PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI- production from AL in the LAB system for PI- polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI+ production from PB in the LAB system for PI+ polar angle from 1.95 to 2.15 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 0.35 to 0.55 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 0.55 to 0.75 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 0.75 to 0.95 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 0.95 to 1.15 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 1.15 to 1.35 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 1.35 to 1.55 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 1.55 to 1.75 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 1.75 to 1.95 radians.
Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 1.95 to 2.15 radians.
A precision measurement of the double-differential production cross-section, ${{d^2 \sigma^{\pi^+}}}/{{d p d\Omega}}$, for pions of positive charge, performed in the HARP experiment is presented. The incident particles are protons of 12.9 GeV/c momentum impinging on an aluminium target of 5% nuclear interaction length. The measurement of this cross-section has a direct application to the calculation of the neutrino flux of the K2K experiment. After cuts, 210000 secondary tracks reconstructed in the forward spectrometer were used in this analysis. The results are given for secondaries within a momentum range from 0.75 GeV/c to 6.5 GeV/c, and within an angular range from 30 mrad to 210 mrad. The absolute normalization was performed using prescaled beam triggers counting protons on target. The overall scale of the cross-section is known to better than 6%, while the average point-to-point error is 8.2%.
Double differential PI+ production cross section in the angular range 30 to 60 mrad.. Errors shown are point-to-point only.
Double differential PI+ production cross section in the angular range 60 to 90 mrad.. Errors shown are point-to-point only.
Double differential PI+ production cross section in the angular range 90 to 120 mrad.. Errors shown are point-to-point only.
Double differential PI+ production cross section in the angular range 120 to 150 mrad.. Errors shown are point-to-point only.
Double differential PI+ production cross section in the angular range 150 to 180 mrad.. Errors shown are point-to-point only.
Double differential PI+ production cross section in the angular range 180 to 210 mrad.. Errors shown are point-to-point only.
We have measured the differential cross section d2σdΩdTπ and the polarization parameter P for the production of π+ and π− in various target nuclei (H1, H2, Be, C, O, Al, Ni, Cu, Mo, and Pb) by protons with a kinetic energy of 585 MeV, for production angles θπ=22.5°, 45°, 60°, 90°, and 135°, and for pion kinetic energies Tπ of 24, 35, 46, 88, 151, 192, and 254 MeV (all quantities in the laboratory system). Our data disagree strongly with recent data for 580-MeV protons. On the other hand, for pion energies up to 150 MeV, our cross sections differ little from those measured for a proton energy of 730 MeV. For nuclei with A>20, the total production cross sections σ(π+) and σ(π−) show the Z13 and N23 proportionality expected from theoretical arguments. There is evidence in our data of a shift of the π+ energy distributions compared to the π− distributions due to the effects of the Coulomb field of the nuclear protons on the emitted pions. NUCLEAR REACTIONS H1, H2, Be, C, O, Al, Ni, Cu, Mo, Pb p, π±, Tp=585 MeV; measured σ(Tπ, θπ) and asymmetry parameter P(Tπ, θπ).
No description provided.
No description provided.
No description provided.
When you search on a word, e.g. 'collisions', we will automatically search across everything we store about a record. But sometimes you may wish to be more specific. Here we show you how.
Guidance on the query string syntax can also be found in the OpenSearch documentation.
We support searching for a range of records using their HEPData record ID or Inspire ID.
About HEPData Submitting to HEPData HEPData File Formats HEPData Coordinators HEPData Terms of Use HEPData Cookie Policy
Status
Email
Forum
Twitter
GitHub
Copyright ~1975-Present, HEPData | Powered by Invenio, funded by STFC, hosted and originally developed at CERN, supported and further developed at IPPP Durham.