No description provided.

Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction P BE --> P X with an 8.9 GeV beam and production angle 105 to 125 degrees.

Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 20 to 30 degrees.

Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 30 to 40 degrees.

Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 40 to 50 degrees.

Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction P BE --> PI+ Xwith an 8.9 GeV beam and production angle 105 to 125 degrees.

Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 20 to 30 degrees.

Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 30 to 40 degrees.

Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 40 to 50 degrees.

Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction P BE --> PI- Xwith an 8.9 GeV beam and production angle 105 to 125 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 20 to 30 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 30 to 40 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 40 to 50 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> P Xwith an 8.9 GeV beam and production angle 105 to 125 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 20 to 30 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 30 to 40 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 40 to 50 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI+ X with an 8.9 GeV beam and production angle 105 to 125 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 20 to 30 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 30 to 40 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 40 to 50 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction PI+ BE --> PI- X with an 8.9 GeV beam and production angle 105 to 125 degrees.

Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 20 to 30 degrees.

Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 30 to 40 degrees.

Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 40 to 50 degrees.

Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction PI- BE --> P Xwith an 8.0 GeV beam and production angle 105 to 125 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 20 to 30 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 30 to 40 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 40 to 50 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI+ X with an 8.0 GeV beam and production angle 105 to 125 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 20 to 30 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 30 to 40 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 40 to 50 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 50 to 60 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 60 to 75 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 75 to 90 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 90 to 105 degrees.

Double differential inclusive cross section for the reaction PI- BE --> PI- X with an 8.0 GeV beam and production angle 105 to 125 degrees.

Ratio of deuteron to proton production in P BE interactions at 8.9 GeV.

Ratio of deuteron to proton production in PI+ BE interactions at 8.9 GeV.

Ratio of deuteron to proton production in PI- BE interactions at 8.0 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 10 (Nrec=90-99).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 10 (Nrec=90-99).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 11 (Nrec=100-109).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 11 (Nrec=100-109).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 12 (Nrec=110-119).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 12 (Nrec=110-119).

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

No description provided.

No description provided.

No description provided.

No description provided.