cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.2211.v1/t56
title: "Table 56" 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/t57
title: "Table 57" 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/t58
title: "Table 58" 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/t59
title: "Table 59" 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/t60
title: "Table 60" 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).
DOI: 10.17182/hepdata.2211.v1/t61
title: "Table 61" 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 = 302.
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/t62
title: "Table 62" 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 = 506.
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/t63
title: "Table 63" 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 = 573.
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/t64
title: "Table 64" 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 = 604.
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/t65
title: "Table 65" 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 = 99.
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/t66
title: "Table 66" 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 = 302.
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/t67
title: "Table 67" 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 = 506.
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/t68
title: "Table 68" 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 = 573.
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/t69
title: "Table 69" 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 = 604.
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/t70
title: "Table 70" 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 = 99.
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/t71
title: "Table 71" 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 = 935.
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/t72
title: "Table 72" 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 = 553.
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/t73
title: "Table 73" 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 = 429.
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/t74
title: "Table 74" 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 = 304.
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/t75
title: "Table 75" 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 = 44.
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/t76
title: "Table 76" 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 = 935.
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/t77
title: "Table 77" 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 = 553.
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/t78
title: "Table 78" 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 = 429.
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/t79
title: "Table 79" 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 = 304.
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/t80
title: "Table 80" 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 = 44.
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.2212.v1/t2
title: "Table 2" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t1
title: "Table 1" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t3
title: "Table 3" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t4
title: "Table 4" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t5
title: "Table 5" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t6
title: "Table 6" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t7
title: "Table 7" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t8
title: "Table 8" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t9
title: "Table 9" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t10
title: "Table 10" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2212.v1/t11
title: "Table 11" of "Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c"

description: No description provided.
description: PLAB=100,150,200 GEV/C. DATA FROM NA3 COLLAB AT CERN ON J/PSI PROD. FOR XF& gt;0. STUDY OF THE A DEPENDENCE SHOWS THAT 18PCT OF PSI`S ARE PRODUCED DIFFRACTIVELY.
DOI: 10.17182/hepdata.2213.v1/t1
title: "Table 1" of "Neutrino and anti-neutrinos Charged Current Inclusive Scattering in Iron in the Energy Range 20-GeV &lt; Neutrino Energy &lt; 300-GeV"

description: ABSOLUTE FLUXES HAVE NOT BEEN MEASURED. NORMALISED TO OLD RESULTS.
description: FINAL DATA ON STRUCTURE FUNCTIONS FROM THE CDHS COLLABORATION. FIRST DATA GIVEN FOR ENERGY DEPENDENCE OF NEUTRINO AND ANTI-NEUTRINO CROSS SECTIONS AND THEN FOR THE STRUCTURE FUNCTIONS F1,F2,F3 IN THE RANGE 1 & lt; Q**2 & lt; 200 GEV**2 , 0.015 & lt; X & lt; 0.65. ANTI-QUARK DISTRIBUTION ALSO ESTIMATED. DATA OBTAINED FROM 200 GEV NARROW-BAND (NEUTRINO AND ANTI -NEUTRINO) AND 300 GEV NARROW-BAND (NEUTRINO ONLY). ALTOGETHER 130,000 NEUTRINO AND 180,000 ANTI-NEUTRINO CHARGED CURRENT EVENTS. THESE DATA SUPERCEED THE OLD DATA (SC=DE GROOT 79. R=ZP C1,143. ) THE TARGET IS AGAIN IRON . THE RADIATIVE CORRECTIONS APPIED ARE DE RUJULA ET AL.
FINAL DATA ON STRUCTURE FUNCTIONS FROM THE CDHS COLLABORATION. FI RST DATA GIVEN FOR ENERGY DEPENDENCE OF NEUTRINO AND ANTI-NEUTRINO CROSS SECTIONS AND THEN FOR THE STRUCTURE FUNCTIONS F1,F2,F3 IN THE RANGE 1 & lt; Q**2 & lt; 200 GEV**2 , 0.015 & lt; X & lt; 0.65. ANTI-QUARK DISTRIBUTION ALSO ESTIMATED. DATA OBTAINED FROM 200 GEVNARROW-BAND (NEUTRINO AND ANTI -NEUTRINO) AND 300 GEV NARROW-BAND (NEUTRINO ONL Y). ALTOGETHER 130,000 NEUTRINO AND 180,000 ANTI-NEUTRINO CHARGED CURRENT EVENTS. THESE DATA SUPERCEED THE OLD DATA (SC=DE GROOT 79. R=ZP C1,143. ) THE TARGET IS AGAIN IRON . THE RADIATIVE CORRECTIONS APPIED ARE DE RUJULA ET AL.
DOI: 10.17182/hepdata.2213.v1/t2
title: "Table 2" of "Neutrino and anti-neutrinos Charged Current Inclusive Scattering in Iron in the Energy Range 20-GeV &lt; Neutrino Energy &lt; 300-GeV"

description: STUCTURE FUNCTIONS ARE EVALUATED ASSUMING R=SIG(L)/SIG(T)=0.1 AND M(W) IS INFINITE. NO CORRECTION FOR FERMI MOTION APPLIED. ERRORS ARE STATISTICAL AND SYSTEMATIC POINT-TO-POINT ERRORS. IN ADDITION OVER-ALL SCALE ERROR OF 6 PCT. FOR F2 , 8 PCT. FOR XF3.
description: FINAL DATA ON STRUCTURE FUNCTIONS FROM THE CDHS COLLABORATION. FIRST DATA GIVEN FOR ENERGY DEPENDENCE OF NEUTRINO AND ANTI-NEUTRINO CROSS SECTIONS AND THEN FOR THE STRUCTURE FUNCTIONS F1,F2,F3 IN THE RANGE 1 & lt; Q**2 & lt; 200 GEV**2 , 0.015 & lt; X & lt; 0.65. ANTI-QUARK DISTRIBUTION ALSO ESTIMATED. DATA OBTAINED FROM 200 GEV NARROW-BAND (NEUTRINO AND ANTI -NEUTRINO) AND 300 GEV NARROW-BAND (NEUTRINO ONLY). ALTOGETHER 130,000 NEUTRINO AND 180,000 ANTI-NEUTRINO CHARGED CURRENT EVENTS. THESE DATA SUPERCEED THE OLD DATA (SC=DE GROOT 79. R=ZP C1,143. ) THE TARGET IS AGAIN IRON . THE RADIATIVE CORRECTIONS APPIED ARE DE RUJULA ET AL.
FINAL DATA ON STRUCTURE FUNCTIONS FROM THE CDHS COLLABORATION. FI RST DATA GIVEN FOR ENERGY DEPENDENCE OF NEUTRINO AND ANTI-NEUTRINO CROSS SECTIONS AND THEN FOR THE STRUCTURE FUNCTIONS F1,F2,F3 IN THE RANGE 1 & lt; Q**2 & lt; 200 GEV**2 , 0.015 & lt; X & lt; 0.65. ANTI-QUARK DISTRIBUTION ALSO ESTIMATED. DATA OBTAINED FROM 200 GEVNARROW-BAND (NEUTRINO AND ANTI -NEUTRINO) AND 300 GEV NARROW-BAND (NEUTRINO ONL Y). ALTOGETHER 130,000 NEUTRINO AND 180,000 ANTI-NEUTRINO CHARGED CURRENT EVENTS. THESE DATA SUPERCEED THE OLD DATA (SC=DE GROOT 79. R=ZP C1,143. ) THE TARGET IS AGAIN IRON . THE RADIATIVE CORRECTIONS APPIED ARE DE RUJULA ET AL.
DOI: 10.17182/hepdata.2213.v1/t3
title: "Table 3" of "Neutrino and anti-neutrinos Charged Current Inclusive Scattering in Iron in the Energy Range 20-GeV &lt; Neutrino Energy &lt; 300-GeV"

description: STUCTURE FUNCTIONS ARE EVALUATED ASSUMING R=SIG(L)/SIG(T)=0.1 AND M(W) IS INFINITE. NO CORRECTION FOR FERMI MOTION APPLIED. ERRORS ARE STATISTICAL AND SYSTEMATIC POINT-TO-POINT ERRORS. IN ADDITION OVER-ALL SCALE ERROR OF 6 PCT. FOR F2 , 8 PCT. FOR XF3.
description: FINAL DATA ON STRUCTURE FUNCTIONS FROM THE CDHS COLLABORATION. FIRST DATA GIVEN FOR ENERGY DEPENDENCE OF NEUTRINO AND ANTI-NEUTRINO CROSS SECTIONS AND THEN FOR THE STRUCTURE FUNCTIONS F1,F2,F3 IN THE RANGE 1 & lt; Q**2 & lt; 200 GEV**2 , 0.015 & lt; X & lt; 0.65. ANTI-QUARK DISTRIBUTION ALSO ESTIMATED. DATA OBTAINED FROM 200 GEV NARROW-BAND (NEUTRINO AND ANTI -NEUTRINO) AND 300 GEV NARROW-BAND (NEUTRINO ONLY). ALTOGETHER 130,000 NEUTRINO AND 180,000 ANTI-NEUTRINO CHARGED CURRENT EVENTS. THESE DATA SUPERCEED THE OLD DATA (SC=DE GROOT 79. R=ZP C1,143. ) THE TARGET IS AGAIN IRON . THE RADIATIVE CORRECTIONS APPIED ARE DE RUJULA ET AL.
FINAL DATA ON STRUCTURE FUNCTIONS FROM THE CDHS COLLABORATION. FI RST DATA GIVEN FOR ENERGY DEPENDENCE OF NEUTRINO AND ANTI-NEUTRINO CROSS SECTIONS AND THEN FOR THE STRUCTURE FUNCTIONS F1,F2,F3 IN THE RANGE 1 & lt; Q**2 & lt; 200 GEV**2 , 0.015 & lt; X & lt; 0.65. ANTI-QUARK DISTRIBUTION ALSO ESTIMATED. DATA OBTAINED FROM 200 GEVNARROW-BAND (NEUTRINO AND ANTI -NEUTRINO) AND 300 GEV NARROW-BAND (NEUTRINO ONL Y). ALTOGETHER 130,000 NEUTRINO AND 180,000 ANTI-NEUTRINO CHARGED CURRENT EVENTS. THESE DATA SUPERCEED THE OLD DATA (SC=DE GROOT 79. R=ZP C1,143. ) THE TARGET IS AGAIN IRON . THE RADIATIVE CORRECTIONS APPIED ARE DE RUJULA ET AL.