cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.2211.v1/t9
title: "Table 9" 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/t16
title: "Table 16" 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/t17
title: "Table 17" 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/t18
title: "Table 18" 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/t20
title: "Table 20" 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/t21
title: "Table 21" 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 = 714.
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/t19
title: "Table 19" 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/t22
title: "Table 22" 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 = 359.
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/t23
title: "Table 23" 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 = 263.
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/t24
title: "Table 24" 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 = 165.
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/t25
title: "Table 25" 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 = 9.
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/t26
title: "Table 26" 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 = 714.
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/t27
title: "Table 27" 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 = 359.
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/t28
title: "Table 28" 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 = 263.
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/t29
title: "Table 29" 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 = 165.
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/t30
title: "Table 30" 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 = 9.
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/t31
title: "Table 31" 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 = 174.
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/t32
title: "Table 32" 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 = 101.
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/t33
title: "Table 33" 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 = 75.
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/t34
title: "Table 34" 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 = 60.
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/t35
title: "Table 35" 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 = 6.
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/t36
title: "Table 36" 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 = 174.
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/t37
title: "Table 37" 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 = 101.
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/t38
title: "Table 38" 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 = 75.
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/t39
title: "Table 39" 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 = 60.
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/t40
title: "Table 40" 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 = 6.
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/t41
title: "Table 41" 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 = 1067.
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/t42
title: "Table 42" 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 = 474.
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/t43
title: "Table 43" 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/t44
title: "Table 44" 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 = 252.
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/t45
title: "Table 45" 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 = 33.
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/t46
title: "Table 46" 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 = 1067.
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/t47
title: "Table 47" 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 = 474.
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/t48
title: "Table 48" 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/t49
title: "Table 49" 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 = 252.
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/t50
title: "Table 50" 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 = 33.
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/t51
title: "Table 51" 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 = 959.
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/t52
title: "Table 52" 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 = 588.
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/t53
title: "Table 53" 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 = 478.
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/t54
title: "Table 54" 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 = 384.
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/t55
title: "Table 55" 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 = 41.
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).