No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

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.

Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 8 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 12 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a P beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for P production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 20 to 30 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 30 to 40 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 40 to 50 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 50 to 60 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 60 to 75 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 75 to 90 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 90 to 105 DEG.

Measured cross section as a function of PT for PI- production from a PI- beam of momentum 15 GeV/c in the angular range 105 to 125 DEG.

The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 20 to 30 DEG.

The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 30 to 45 DEG.

The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 45 to 65 DEG.

The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 65 to 90 DEG.

The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 90 to 125 DEG.

THE EVENTS WITHOUT BACKWARD PROTONS.

THE EVENTS WITH BACKWARD PROTONS.

THE EVENTS WITHOUT BACKWARD PROTONS.

THE EVENTS WITHT BACKWARD PROTONS.

No description provided.

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.

No description provided.

No description provided.

No description provided.

No description provided.

RUN 2.

RUN 2.

RUN 2.

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.

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.