X ERROR TARG.THICKN. = 0.10 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.10 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.19 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.19 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.19 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.24 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.24 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.24 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.24 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.24 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.57 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

X ERROR TARG.THICKN. = 0.57 RAD.LENGTH. X ERROR D(THETA) = 0.3000 MRAD.

No description provided.

Axis error includes +- 0.0/0.0 contribution (?////DUE TO ABSORPTION CORRECTIONS//THE CORRECTION TO THE RATIO DEUT/P DUE TO DIFFERENCE OF PARTICLE ABSORPTION IN CHERENKOV COUNTERS WERE DETERMINED EXPERIMENTALLY (IN THE RANGE 6-45 PCT). THERE WAS THE CORRECTION OF ABOUT 19 PCT FOR ABSORPTION IN THE OTHER PARTS OF THE SPECTROMETER).

Axis error includes +- 0.0/0.0 contribution (?////DUE TO ABSORPTION CORRECTIONS//THE CORRECTION TO THE RATIO DEUT/P DUE TO DIFFERENCE OF PARTICLE ABSORPTION IN CHERENKOV COUNTERS WERE DETERMINED EXPERIMENTALLY (IN THE RANGE 6-45 PCT). THERE WAS THE CORRECTION OF ABOUT 19 PCT FOR ABSORPTION IN THE OTHER PARTS OF THE SPECTROMETER).

Axis error includes +- 0.0/0.0 contribution (?////DUE TO ABSORPTION CORRECTIONS//THE CORRECTION TO THE RATIO DEUT/P DUE TO DIFFERENCE OF PARTICLE ABSORPTION IN CHERENKOV COUNTERS WERE DETERMINED EXPERIMENTALLY (IN THE RANGE 6-45 PCT). THERE WAS THE CORRECTION OF ABOUT 19 PCT FOR ABSORPTION IN THE OTHER PARTS OF THE SPECTROMETER).

Axis error includes +- 0.0/0.0 contribution (?////DUE TO ABSORPTION CORRECTIONS//THE CORRECTION TO THE RATIO DEUT/P DUE TO DIFFERENCE OF PARTICLE ABSORPTION IN CHERENKOV COUNTERS WERE DETERMINED EXPERIMENTALLY (IN THE RANGE 6-45 PCT). THERE WAS THE CORRECTION OF ABOUT 19 PCT FOR ABSORPTION IN THE OTHER PARTS OF THE SPECTROMETER).

Axis error includes +- 0.0/0.0 contribution (?////DUE TO ABSORPTION CORRECTIONS//THE CORRECTION TO THE RATIO DEUT/P DUE TO DIFFERENCE OF PARTICLE ABSORPTION IN CHERENKOV COUNTERS WERE DETERMINED EXPERIMENTALLY (IN THE RANGE 6-45 PCT). THERE WAS THE CORRECTION OF ABOUT 19 PCT FOR ABSORPTION IN THE OTHER PARTS OF THE SPECTROMETER).

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

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.

DATA FOR P DEUT INTERACTIONS ARE PRESENTED BY THE AUTHORS IN THE PAPER YF 31, 1483, (1980).

DATA FOR P DEUT INTERACTIONS ARE PRESENTED BY THE AUTHORS IN THE PAPER YF 31, 1483.

DATA FOR P DEUT INTERACTIONS ARE PRESENTED BY THE AUTHORS IN THE PAPER YF 31, 1483.

DATA FOR P DEUT INTERACTIONS ARE PRESENTED BY THE AUTHORS IN THE PAPER YF 31, 1483.

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.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

$p_{\rm T}$-differential yield of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity class).

$p_{\rm T}$-differential yield of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity class).

$p_{\rm T}$-differential yield of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity class).

$p_{\rm T}$-differential yield of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100multiplicity class).

$p_{\rm T}$-differential invariant yield of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD). Additional systematic error: +- 3.1% (normalization).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-5% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (5-10% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (10-20% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100% multiplicity class).

$p_{\rm T}$-integrated yield d$N$/d$y$ of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case (additional normalization systematic error: +- 3.1%).

Mean $p_{\rm T}$ of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

$p_{\rm T}$-integrated yield d$N$/d$y$ of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case (additional normalization systematic error: +- 3.1%).

Mean $p_{\rm T}$ of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

Mean $p_{\rm T}$ as function of the mass for particles measured with the ALICE detector in INEL pp collisions at $\sqrt{s}$ = 7 TeV in |y| < 0.5.

Mean $p_{\rm T}$ as function of the mass for particles measured with the ALICE detector in 0-20% p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in -0.5 < y < 0.

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-5$\%$ multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (5-10% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (10-20% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100% multiplicity class).

Ratio of $p_{\rm T}$-integrated yields of $(K^{*0}+\overline{K^{*0}})$ to long lived hadrons for different V0A multiplicity classes in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Ratio of $p_{\rm T}$-integrated yields of 2$\phi$ to long lived hadrons for different V0A multiplicity classes in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV.