Differential cross section for proton production with a negative pion beam and Beryllium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Beryllium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Beryllium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Beryllium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Beryllium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Beryllium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Beryllium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Beryllium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Beryllium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Carbon target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Carbon target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Carbon target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Carbon target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Carbon target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Carbon target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Carbon target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Carbon target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Carbon target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Carbon target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Carbon target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Carbon target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Aluminium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Aluminium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Aluminium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Aluminium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Aluminium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Aluminium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Aluminium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Aluminium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Copper target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Copper target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Copper target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Copper target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Copper target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Copper target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Copper target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Copper target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Copper target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Copper target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Copper target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Copper target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Tin target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Tin target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Tin target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Tin target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Tin target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Tin target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Tin target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Tin target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Tin target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Tin target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Tin target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Tin target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Tantallum target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Tantallum target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Tantallum target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Tantallum target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Tantallum target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Tantallum target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Tantallum target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Tantallum target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Tantallum target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Tantallum target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Tantallum target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Tantallum target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Lead target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Lead target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Lead target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a negative pion beam and Lead target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Lead target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Lead target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Lead target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a positive pion beam and Lead target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Lead target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Lead target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Lead target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Differential cross section for proton production with a proton beam and Lead target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 3 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 5 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 8 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 12 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in P PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI+ PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for P production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI+ production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 20 to 30 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 30 to 40 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 40 to 50 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 50 to 60 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 60 to 75 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 75 to 90 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 90 to 105 degrees.

Double-differential inclusive cross section for PI- production in PI- PB interactions at beam momentum 15 GeV/c in the polar angle range 105 to 125 degrees.

CYCLE N2.

CYCLE N2.

CYCLE N2.

CYCLE N2.

No description provided.

CYCLE N2.

CYCLE N2.

CYCLE N2.

CYCLE N2.

CYCLE N2.

CYCLE N2.

CYCLE N2.

FOR AL, CU, PB, TARGETS HI2/D.O.F.=1,FOR BE TARGET HI2/D.O.F.=3.2.

FOR AL, CU, PB, TARGETS HI2/D.O.F.=1,FOR BE TARGET HI2/D.O.F.=3.2.

FOR AL, CU, PB, TARGETS HI2/D.O.F.=1,FOR BE TARGET HI2/D.O.F.=3.2.

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RUN 2.

RUN 2.

RUN 2.

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THE EVENTS WITHOUT BACKWARD PROTONS.

THE EVENTS WITH BACKWARD PROTONS.

THE EVENTS WITHOUT BACKWARD PROTONS.

THE EVENTS WITHT BACKWARD PROTONS.

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