cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.2143.v1/t10
title: "Table 10" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t11
title: "Table 11" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t12
title: "Table 12" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t13
title: "Table 13" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t8
title: "Table 8" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: No description provided.
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t9
title: "Table 9" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: No description provided.
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t14
title: "Table 14" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t15
title: "Table 15" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t16
title: "Table 16" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t17
title: "Table 17" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t18
title: "Table 18" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t19
title: "Table 19" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t20
title: "Table 20" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t21
title: "Table 21" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t22
title: "Table 22" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t23
title: "Table 23" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t24
title: "Table 24" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t25
title: "Table 25" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t26
title: "Table 26" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2143.v1/t27
title: "Table 27" of "Charged Hadron Composition of the Final State in e+ e- Annihilation at High-Energies"

description: Axis error includes +- 0.0/0.0 contribution (?////EXCEPT OVERALL NORMALIZATION).
description: DESY-PETRA. TASSO COLLABORATION. THE PRESENT DATA IS AN EXTENSION OF THAT PRESENTED IN BRANDELIK ET AL., PL 113B, 98 (1982). AT W=14 AND 22 GEV, DATA SAMPLES IDENTICAL TO THOSE IN THE ABOVE REFERENCE ARE USED TO DETERMINE THE K+, K- AND P, AP YIELDS. AT W=34 GEV, IN ADDITION TO MEASURING THE K+, K- AND P, AP YIELDS, THE ANALYSIS FOR PI+, PI- HAS BEEN REPEATED WITH A DATA SAMPLE OF APPROX. TWICE THE SIZE USED IN THE ABOVE REFERENCE. THE SCALING VARIABLE IS X(P=3,DEF=2*E(P=3)/SQRT(X)) AND BETA IS P(P=3)/E(P=3).
DOI: 10.17182/hepdata.2210.v1/t1
title: "Table 1" of "QUASIELASTIC PRODUCTION OF LAMBDA HYPERON IN ANTI-NEUTRINO INTERACTIONS AT HIGH-ENERGIES"

description: No description provided.
description: DATA WERE ALREADY PUBLISHED IN IFVE-86-95 (NOT SUBMITTED TO ZETFP).
DATA WERE ALREADY PUBLISHED IN IFVE-86-95 (NOT SUBMITTED TO ZETFP). DATA REQUESTED 1 APR 1987 BY YGS.
DOI: 10.17182/hepdata.2210.v1/t2
title: "Table 2" of "QUASIELASTIC PRODUCTION OF LAMBDA HYPERON IN ANTI-NEUTRINO INTERACTIONS AT HIGH-ENERGIES"

description: No description provided.
description: DATA WERE ALREADY PUBLISHED IN IFVE-86-95 (NOT SUBMITTED TO ZETFP).
DATA WERE ALREADY PUBLISHED IN IFVE-86-95 (NOT SUBMITTED TO ZETFP). DATA REQUESTED 1 APR 1987 BY YGS.
DOI: 10.17182/hepdata.2211.v1/t1
title: "Table 1" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 971.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t2
title: "Table 2" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 1628.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t3
title: "Table 3" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 2135.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t5
title: "Table 5" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 321.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t4
title: "Table 4" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 1916.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t6
title: "Table 6" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 971.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t7
title: "Table 7" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 1628.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t10
title: "Table 10" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 321.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t11
title: "Table 11" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 1564.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t12
title: "Table 12" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 754.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t13
title: "Table 13" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 502.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t14
title: "Table 14" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 343.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t15
title: "Table 15" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 62.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).
DOI: 10.17182/hepdata.2211.v1/t8
title: "Table 8" of "Rapidity Distributions of Ca + Ca, Nb + Nb, Ne + Au, and Au + Au at Bombarding Energies From 250-{MeV} to 2100-{MeV}/nucleon"

description: THE STATISTICAL ERROR OF THE DATA CAN BE OBTAINED AS SQRT(D(N)/ D(YRAP)/NF) WHERE THE NORMALIZATION FACTOR NF = 2135.
description: BERKELEY BEVALAC, PLACTIC BALL/WALL SPECTROMETER. BECAUSE OF COMPLEX ACCEPTANCE OF THE PLASTIC A FORTRAN PROGRAM WAS WRITTEN TO FILTER THE OUTPUT OF SIMULATIONS SO THAT CAN BE COMPARED WITH OUT DATA. THE CODE IS AVAILABLE FROM THE AUTHORS (ON E-MAIL FROM POSKA@LBL).