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CONTENTS
HEPDATA
ON-LINE
DATA
REVIEW
A Review of Quarkonii Data
in Hadronic Interactions
.
HEPDATA
ON-LINE
DATA
REVIEW
Experiments
CERNS-SPS
NA3 NA10
NA11 NA16
NA27 NA32
NA34-3(HELIOS)
NA38 NA50
NA51 NA60
CERN-SppS
UA1 UA6
DESY-HERA
HERA-B
BNL-RHIC
PHENIX STAR
Fermilab-Tevatron
CDF D0
E772 E789
E866
CERN-LHC
ALICE ATLAS
CMS LHCb
Initial States
p(bar)-p
p-d p-A
d-A A-A
meson-p(A)
Measurements
Cross Sections
Total
Differential(Y)
Differential(PT)
Differential(X)
Polarization
Final States
J/PSI PSI
CHI/C Upsilon
D/D* DiMuon
Charm Beauty
Lambda/C Xi/C
QUARKONII data
Data for P(BAR)_NUCLEUS interactions BACK

The individual links display the specific datasets.
The publication reference link displays the SPIRES hep database entry.
The [R] link displays the complete entry for that paper from the HepData Reaction database.
HERAB - E866 - E789 - E772 - NA3 - NA32 - NA34-3 - NA38 - NA50 -

HERAB

  • Abt et al. EPJ C26(2003)345 [R] - 4951484
    Measurement of the b anti-b production cross-section in 920-GeV fixed target proton nucleus collisions
    • - p A --> B... 920 GeV
      SIG v DECAY (1)(The measured cross section for the E+ E- and MU+ MU- channels separately.... NUCLEON,C,Ti)
      SIG v XL (2)(The measured and extrapolated combined B-BBAR production cross section.... NUCLEON,C,Ti)
  • Abt et al. PL B561(2002)61 [R] - 5378796
    $J/\\psi$ production via chi($c$) decays in 920-GeV pA interactions
    • - p A --> J/PSI,CHI... 920 GeV
      SIG v DECAY (1)(Ratio of CHIC to J/PSI production cross section in P C interactions for the E+ E... NUCLEON,C,Ti)
      SIG v DECAY (2)(Ratio of CHI/C to J/PSI production cross section in P TI interactions for the E+... NUCLEON,C,Ti)
      SIG v PLAB (3)(Averaged ratio of CHIC to J/PSI production cross section in P C and P Ti interac... NUCLEON,C,Ti)
      SIG v PLAB (4)(Ratio of direct CHIC to direct J/PSI production cross section in P C and P Ti in... NUCLEON,C,Ti)
  • Abt et al. PL B596(2004173) [R] - 5882770
    Search for the flavor changing neutral current decay D0 ---> mu+ mu- with the HERA-B detector
    • - p A --> D... 920 GeV
      SIG v PLAB (1)(Upper limit on the branching fraction of D0 --> MU+ MU- in P NUCLEON interact... NUCLEON,C,Ti)
  • Abt et al. PL B638(2006)407 [R] - 6454720
    Measurement of the $J/\\psi$ production cross section in 920-GeV/c fixed-target proton-nucleus interactions
    • - p A --> J/PSI... 920 GeV
      SIG v RE (1)(Cross section for the individual targets for the visible rapidity region.... NUCLEON,C,Ti,Wt)
      SIG v RE (2)(Total cross section for the individual targets extrapolated to the full phase sp... NUCLEON,C,Ti,Wt)
      SIG v PLAB (3)(Total cross section for P NUCLEON --> J/PSI X for the full phase space.... NUCLEON,C,Ti,Wt)
    • - p A --> J/PSI... 920 GeV
      DSIG/DYRAP v PLAB (4)(Differential cross section at rapidity zero for P NUCLEON --> J/PSI X.... NUCLEON,C,Ti,Wt)
  • Abt et al. PR D73(2006)052005 [R] - 6454739
    Improved measurement of the b-anti-b production cross section in 920-GeV fixed-target proton-nucleus collisions
    • - p A --> B,J/PSI... 920 GeV
      SIG v DECAY (1)(Ratio of prompt J/PSI to B-BBAR production cross section in P C interactions in ... NUCLEON,C,Ti,Wt)
      SIG v DECAY (2)(Ratio of prompt J/PSI to B-BBAR production cross section in P TI interactions i... NUCLEON,C,Ti,Wt)
      SIG v DECAY (3)(Ratio of prompt J/PSI to B-BBAR production cross section in P WT interactions in... NUCLEON,C,Ti,Wt)
      SIG v DECAY (4)(Ratio of prompt J/PSI to B-BBAR production cross section in P NUCLEON interactio... NUCLEON,C,Ti,Wt)
      SIG v PLAB (5)(Ratio of combined prompt J/PSI to B-BBAR production cross section in P NUCLEON i... NUCLEON,C,Ti,Wt)
      SIG v PLAB (6)(Measured value of the B-BBAR cross section extrapolated to the full phase space.... NUCLEON,C,Ti,Wt)
      SIG v PLAB (7)(Measured value of the B-BBAR cross section extrapolated to the full phase space.... NUCLEON,C,Ti,Wt)
  • Abt et al. PL B638(2006)13 [R] - 6553958
    Measurement of the $\\upsilon$ production cross-section in 920-GeV fixed-target proton-nucleus collisions
    • - p A --> J/PSI,UPSI... 920 GeV
      SIG v DECAY (1)(Ratio of the UPSILON production cross section to the total J/PSI production cro... NUCLEON)
      SIG v RE (2)(UPSILON production cross section at midrapidity in P NUCLEON interactions for th... NUCLEON)
    • - p A --> UPSI... 920 GeV
      SIG v DECAY (1)(Ratio of the UPSILON production cross section to the total J/PSI production cro... NUCLEON)
      SIG v RE (2)(UPSILON production cross section at midrapidity in P NUCLEON interactions for th... NUCLEON)
  • Abt et al. EPJ C49(2006)545 [R] - 6853218
    A Measurement of the $\\psi^\\prime$ to $J/\\psi$ production ratio in 920-GeV proton-nucleus interactions
    • - p A --> PSI... 920 GeV
      SIG/SIG v COS (1)(Ratio of PSI(3685) and J/PSI cross sections for both muon and electron channels ... NUCLEUS,C,Ti,Wt)
      SIG/SIG v PT (2)(Ratio of PSI(3685) and J/PSI cross sections for both muon and electron channels ... NUCLEUS,C,Ti,Wt)
    • - p A --> J/PSI... 920 GeV
      SIG/SIG v COS (1)(Ratio of PSI(3685) and J/PSI cross sections for both muon and electron channels ... NUCLEUS,C,Ti,Wt)
      SIG/SIG v PT (2)(Ratio of PSI(3685) and J/PSI cross sections for both muon and electron channels ... NUCLEUS,C,Ti,Wt)
  • Abt et al. PL B650(2006)103 [R] - 7009216
    Bottom production cross-section from double muonic decays of b-flavoured hadrons in 920-GeV proton-nucleus collision
    • - p A --> B... 920 GeV
      SIG v Ecm (2)(BOTTOM BOTTOMBAR production cross section combined with previous HERA-B measurem... NUCLEUS,C,Ti,Wt)
      SIG v Ecm (1)(BOTTOM BOTTOMBAR production cross section... NUCLEUS,C,Ti,Wt)
  • Abt et al. EPJ C52(2007)531 [R] - 7297750
    Measurement of D0, D+, D+(s) and D*+ Production in Fixed Target 920-GeV Proton-Nucleus Collisions
    • - p A --> D... 920 GeV
      SIG v RE (1)(Cross sections (micro barns) in the visible range (-0.15<x_F<0.05).... Nucleus,C,Ti,Wt)
      SIG v RE (2)(Cross sections (micro barns) extrapolated to the total phase space.... Nucleus,C,Ti,Wt)
      SIG v RE (3)(Cross sections(micro barns) for particles production in the visible range (-0.1... Nucleus,C,Ti,Wt)
      SIG v RE (4)(Cross sections(micro barns) for anti-particle production in the visible range (-... Nucleus,C,Ti,Wt)
      SIG v RE (5)(Visible cross sections per nucleus(mb).... Nucleus,C,Ti,Wt)
      SIG v Ecm (7)(Leading to non-leading particle asymmetries A in the visible range, -0.15<x_F... Nucleus,C,Ti,Wt)
    • - p A --> D... 920 GeV
      SIG/SIG v Ecm (6)(Ratios of cross sections.... NUCLEUS,C,Ti,Wt)
  • Abt et al. PR D79(2008)012001 [R] - 7828845
    Production of the Charmonium States $\\chi_{c1}$ and $\\chi_{c2}$ in Proton Nucleus Interactions at $\\sqrt{s}$ = 41.6-GeV
    • - p A --> J/PSI,CHI... 920 GeV
      SIG/SIG v NUCLEUS (1)(Measurement of R_CHI/C in <E+ E->, <MU+ MU-> and combined channel... NUCLEUS,C,Ti,Wt)
      SIG/SIG v NUCLEUS (2)(Measurement of R_12 in <E+ E->, <MU+ MU-> and combined channel... NUCLEUS,C,Ti,Wt)
      SIG/SIG v NUCLEUS (3)(Measurement of SIG(C1)/SIG(C2) in <E+ E->, <MU+ MU-> and combined ch... NUCLEUS,C,Ti,Wt)
  • Abt et al. EPJ C60(2008)525 [R] - 8075050
    Kinematic distributions and nuclear effects of J/psi production in 920-GeV fixed-target proton-nucleus collisions
    • - p A --> J/PSI... 920 GeV
      DN/DPT v PT (1)(J/PSI distributions (dN/dp_T, normalized to their integrals over the measured ra... NUCLEUS,C,Ti,Wt)
    • - p A --> J/PSI... 920 GeV
      DN/DXF v XF (2)(J/PSI distributions (dN/dx_F, normalized to their integrals over the measured ra... NUCLEUS,C,Ti,Wt)
    • - p A --> J/PSI... 920 GeV
      POWER v XF (4)(The parameter Alpha as a function of x_F. Statistical and systematic uncertainti... NUCLEUS,C,Ti,Wt)
      POWER v PT (3)(The parameter Alpha as a function of p_T. Statistical and systematic uncertainti... NUCLEUS,C,Ti,Wt)
  • Abt et al. EPJ C60(2009)517 [R] - 8113157
    Angular distributions of leptons from $J/\\psi$ ' $s$ produced in 920 GeV fixed-target proton-nucleus collisions
    • - p A --> J/PSI... 920 GeV
      POL v MEAN(NAME=XF) (9)(Values of the parameters Lambda_theta measured in the Collins-Soper frame as a f... NUCLEUS,C,Wt)
      POL v MEAN(NAME=PT) (8)(Values of the parameters Lambda_theta measured in the Collins-Soper frame as a f... NUCLEUS,C,Wt)
      POL v MEAN(NAME=XF) (7)(Values of the parameters Lambda_theta, Lambda_phi et Lambda_theta_phi measured i... NUCLEUS,C,Wt)
      POL v MEAN(NAME=PT) (6)(Values of the parameters Lambda_theta, Lambda_phi et Lambda_theta_phi measured i... NUCLEUS,C,Wt)
      POL v MEAN(NAME=XF) (5)(Values of the parameters Lambda_theta, Lambda_phi et Lambda_theta_phi measured i... NUCLEUS,C,Wt)
      POL v MEAN(NAME=PT) (4)(Values of the parameters Lambda_theta, Lambda_phi et Lambda_theta_phi measured i... NUCLEUS,C,Wt)
      POL v MEAN(NAME=XF) (3)(Values of the parameters Lambda_theta, Lambda_phi et Lambda_theta_phi measured i... NUCLEUS,C,Wt)
      POL v YN (2)(Values of the parameters Lambda_theta, Lambda_phi et Lambda_theta_phi measured i... NUCLEUS,C,Wt)
      POL v YN (1)(Output parameters obtained by fitting the distributions... NUCLEUS,C,Wt)
E866
  • Leitch et al. PRL 84(2000)3256 [R] - 4188497
    Measurement of J / psi and psi-prime suppression in p-A collisions at 800-GeV/c
    • - p A --> J/PSI... 800 GeV
      POWER v MEAN(PT) (5)(PT dependence of ALPHA for J/PSI and PSIPRIME production for the large-XF datase... Be,Fe,Wt)
      POWER v MEAN(PT) (4)(PT dependence of ALPHA for J/PSI and PSIPRIME production for the intermediate-XF... Be,Fe,Wt)
      POWER v MEAN(PT) (3)(PT dependence of ALPHA for J/PSI and PSIPRIME production for the small-XF datase... Be,Fe,Wt)
      POWER v MEAN(XL) (2)(Target Atomic Mass dependence expressed as the POWER for PSIPRIME production. X2... Be,Fe,Wt)
      POWER v MEAN(XL) (1)(Target Atomic Mass dependence expressed as the POWER for J/PSI production. X2 is... Be,Fe,Wt)
    • - p A --> PSI... 800 GeV
      POWER v MEAN(PT) (5)(PT dependence of ALPHA for J/PSI and PSIPRIME production for the large-XF datase... Be,Fe,Wt)
      POWER v MEAN(PT) (4)(PT dependence of ALPHA for J/PSI and PSIPRIME production for the intermediate-XF... Be,Fe,Wt)
      POWER v MEAN(PT) (3)(PT dependence of ALPHA for J/PSI and PSIPRIME production for the small-XF datase... Be,Fe,Wt)
      POWER v MEAN(XL) (2)(Target Atomic Mass dependence expressed as the POWER for PSIPRIME production. X2... Be,Fe,Wt)
      POWER v MEAN(XL) (1)(Target Atomic Mass dependence expressed as the POWER for J/PSI production. X2 is... Be,Fe,Wt)
  • Brown et al. PRL 86(2001)2529 [R] - 4499042
    Observation of polarization in bottomonium production at s**(1/2) = 38.8-GeV
    • - p A --> MU... 800 GeV
      POL v PT (1)(The observed polarization in the Drell-Yan sideband region as a function of PT. ... Cu)
      POL v XL (2)(The observed polarization in the Drell-Yan sideband region as a function of XL. ... Cu)
      POL v PT (3)(The observed polarization in the UPSILON(1S) region as a function of PT. There i... Cu)
      POL v XL (4)(The observed polarization in the UPSILON(1S) region as a function of XL. There i... Cu)
      POL v PT (5)(The observed polarization in the UPSILON(2S) + UPSILON(3S) region as a function ... Cu)
      POL v XL (6)(The observed polarization in the UPSILON(2S) + UPSILON(3S) region as a function ... Cu)
    • - p A --> UPSI... 800 GeV
      POL v PT (1)(The observed polarization in the Drell-Yan sideband region as a function of PT. ... Cu)
      POL v XL (2)(The observed polarization in the Drell-Yan sideband region as a function of XL. ... Cu)
      POL v PT (3)(The observed polarization in the UPSILON(1S) region as a function of PT. There i... Cu)
      POL v XL (4)(The observed polarization in the UPSILON(1S) region as a function of XL. There i... Cu)
      POL v PT (5)(The observed polarization in the UPSILON(2S) + UPSILON(3S) region as a function ... Cu)
      POL v XL (6)(The observed polarization in the UPSILON(2S) + UPSILON(3S) region as a function ... Cu)
  • Chang et al. PRL 91(2003)21108 - 5625602

    • - p A --> J/PSI... 800 GeV
E789
  • Kowitt et al. PRL 72(1994)1318 [R] - 2860015
    Production of J / psi at large x(F) in 800-GeV/c p copper and p beryllium collisions
    • - p A --> J/PSI... 800 GeV
      DSIG/DXL v XL (1)(Location: T 1,F 2... Cu,Be)
      DSIG/DXL v XL (2)(Location: T 1,F 2... Cu,Be)
    • - p A --> J/PSI... 800 GeV
  • Leitch et al. PRL 72(1994)2542 [R] - 2907631
    Nuclear dependence of neutral D meson production by 800-GeV/c protons
    • - p A --> D... 800 GeV
      SIG v PLAB (5)(PT and XL parametrization from PL 263B, 573 and PRL 61, 2185 are used. This resu... Nucleus,Nucleon,Au,Be)
      SIG v PLAB (3)(... Nucleus,Nucleon,Au,Be)
      SIG v PLAB (1)(... Nucleus,Nucleon,Au,Be)
    • - p A --> D... 800 GeV
      POWER v PT (8)(... Nucleus,Nucleon,Au,Be)
      POWER v XL (7)(... Nucleus,Nucleon,Au,Be)
      POWER v PLAB (2)(... Nucleus,Nucleon,Au,Be)
    • - p A --> D... 800 GeV
      DSIG/DPT**2 v PLAB (6)(... Nucleus,Nucleon,Au,Be)
    • - p A --> D... 800 GeV
      DSIG/DXL v XL (4)(... Nucleus,Nucleon,Au,Be)
  • Jansen et al. PRL 74(1994)3118 [R] - 3087840
    Measurement of the bottom quark production cross-section in 800-GeV/c proton - gold collisions
    • - p A --> J/PSI... 800 GeV
      SIG v PT (3)(All J/PSI(1S) are from B/BBAR decays. Cross section per nucleon was obtained wit... Nucleon,Be,Ci,Wt)
      SIG v PLAB (2)(Cross section per nucleon was obtained with linear A-dependence... Nucleon,Be,Ci,Wt)
    • - p A --> B... 800 GeV
      SIG v PT (3)(All J/PSI(1S) are from B/BBAR decays. Cross section per nucleon was obtained wit... Nucleon,Be,Ci,Wt)
      SIG v PLAB (2)(Cross section per nucleon was obtained with linear A-dependence... Nucleon,Be,Ci,Wt)
    • - p A --> J/PSI... 800 GeV
      D2SIG/DPT**2/DXL v XL (1)(All J/PSI(1S) are from B/BBAR decays. Cross section per nucleon was obtained wit... Nucleon,Be,Ci,Wt)
  • Schub et al. PR D52(1995)1307 [R] - 3130991
    Measurement of J / psi and psi-prime production in 800-GeV/c proton - gold collisions
  • Leitch et al. PR D52(1995)4251 [R] - 3127230
    Nuclear dependence of J / psi production by 800-GeV/c protons near x(F) = 0
  • Misha et al. PR D50(1994)9 [R] - 2952050
    Search for the decay D0 ---> mu+ mu-
    • - p A --> D... 800 GeV
      SIG/SIG v PLAB (2)(Classical 90 PCT upper limit of branching ratio.... Pt)
      SIG/SIG v PLAB (1)(Measured branching ratio.... Pt)
E772
  • Alde et al. PRL 64(1990)2479 [R] - 2317567
    Nuclear dependence of dimuon production at 800-GeV. FNAL-772 experiment
    • - p A --> MU... 800 GeV
      SIG v M (4)(Ratio of dimuon yield per nucleon for FE/H2... Fe)
      SIG v PT (5)(Ratio of dimuon yield per nucleon for FE/H2... Fe)
      SIG v XL (6)(Ratio of dimuon yield per nucleon for FE/H2... Fe)
      SIG v XT (9)(Ratios of DY dimuon yields per nucleon as a function of XT for positive XF.... Fe)
    • - p A --> MU... 800 GeV
      SIG v XT (7)(Ratios of DY dimuon yields per nucleon as a function of XT for positive XF.... C)
    • - p A --> MU... 800 GeV
      SIG v XT (8)(Ratios of DY dimuon yields per nucleon as a function of XT for positive XF.... Ca)
    • - p A --> MU... 800 GeV
      SIG v XT (10)(Ratios of DY dimuon yields per nucleon as a function of XT for positive XF.... Wt)
  • Alde et al. PRL 66(1991)133 [R] - 2280019
    The A-dependence of J / psi and psi-prime production at 800-GeV/c
    • - p A --> J/PSI... 800 GeV
      SIG v A (1)(Ratio of heavy nucleus to deuterium yields. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v A (2)(Ratio of heavy nucleus to deuterium yeilds. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v A (3)(Ratio of heavy nucleus to deuterium yeilds. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v PT (4)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v PT (5)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v XL (6)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v XL (7)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
    • - p A --> PSI... 800 GeV
      SIG v A (1)(Ratio of heavy nucleus to deuterium yields. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v A (2)(Ratio of heavy nucleus to deuterium yeilds. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v A (3)(Ratio of heavy nucleus to deuterium yeilds. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v PT (4)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v PT (5)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v XL (6)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v XL (7)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
    • - p A --> MU... 800 GeV
      SIG v A (1)(Ratio of heavy nucleus to deuterium yields. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v A (2)(Ratio of heavy nucleus to deuterium yeilds. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v A (3)(Ratio of heavy nucleus to deuterium yeilds. A is the mass number of the target n... Nucleus,D,C,Ca,Fe,Wt)
      SIG v PT (4)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v PT (5)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v XL (6)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
      SIG v XL (7)(Location: F 2... Nucleus,D,C,Ca,Fe,Wt)
    • - p A --> J/PSI... 800 GeV
      POWER v XL (8)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v XL (9)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v PT (10)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v PT (11)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v X2 (12)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v X2 (13)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
    • - p A --> MU... 800 GeV
      POWER v XL (8)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v XL (9)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v PT (10)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v PT (11)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v X2 (12)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
      POWER v X2 (13)(Cross section parametrised as sig(mass**ALPHA). ALPHA is coded here as POWER(N=A... Nucleus,D,C,Ca,Fe,Wt)
  • Alde et al. PRL 66(1991)2285 [R] - 2342618
    Nuclear dependence of the production of Upsilon resonances at 800-GeV
    • - p A --> UPSI... 800 GeV
      SIG v XL (7)(Ratio of yields per nucleon as a function of feynman X. These data were supplied... Nucleus,D,C,Ca,Fe,Wt)
      SIG v PT (8)(Ratio of yields per nucleon as a function of transverse momentum. These data wer... Nucleus,D,C,Ca,Fe,Wt)
    • - p A --> UPSI... 800 GeV
      POWER v XL (1)(Mass dependence as a function of feynman X for UPSI(1S) production.... Nucleus,D,C,Ca,Fe,Wt)
      POWER v XL (2)(Mass dependence as a function of feynman X for UPSI(2S/3S) production.... Nucleus,D,C,Ca,Fe,Wt)
      POWER v PT (3)(Mass dependence as a function of transverse momentum for UPSI(1S) production.... Nucleus,D,C,Ca,Fe,Wt)
      POWER v PT (4)(Mass dependence as a function of transverse momentum for UPSI(2S/3S) production.... Nucleus,D,C,Ca,Fe,Wt)
      POWER v X2 (5)(Mass dependence as a function of the momentum fraction of the struck quark X2 fo... Nucleus,D,C,Ca,Fe,Wt)
      POWER v X2 (6)(Mass dependence as a function of the momentum fraction of the struck quark X2 fo... Nucleus,D,C,Ca,Fe,Wt)
NA3
  • Badier et al. ZP C20(1983)101 [R] - 1089439
    Experimental J/psi Hadronic Production from 150-GeV/c to 280-GeV/c
    • - p A --> J/PSI... 150,200,280 GeV
      SIG v XL (4)(Location: T 5... Nucleus,p,Pt)
      SIG v P (7)(Location: 7... Nucleus,p,Pt)
    • - pbar A --> J/PSI... 150,200,280 GeV
      SIG v XL (3)(Location: T 5... Nucleus,p,Pt)
      SIG v P (6)(Location: 6... Nucleus,p,Pt)
  • Badier et al. PL 158B(1985)85 [R] - 1351532
    psi psi PRODUCTION AND LIMITS ON BEAUTY MESON PRODUCTION FROM 400-GeV/c PROTONS
    • - p A --> J/PSI... 400 GeV
      SIG v P (1)(Location: 1... Nucleus,Pt)
NA32
  • Bailey et al. NP B239(1984)15 [R] - 1133390
    UPPER LIMITS FOR CHARM PRODUCTION IN 150-GeV p Be INTERACTIONS
    • - p A --> CHARM... 150 GeV
      SIG v P (1)(Location: 1... Be,Nucleon)
NA34-3
  • Angelis et al. EJP C13(1998)433 [R] - 3774848
    Excess of continuum dimuon production at masses between threshold and the J / Psi in S - W interactions at 200-GeV/c/nucleon
    • - p WT --> MU... 200 GeV
      N v M (1)(Location: T 2... -)
      N v M (3)(Location: T 3... -)
      N v M (5)(Location: T 4... -)
      N v M (7)(Location: T 6... -)
NA38
  • Baglin et al. PL 262B(1991)362 [R] - 2461196
    Transverse momentum of J / psi produced in p Cu, p U, O-16 Cu, O-16 U and S-32 U collisions at 200-GeV per nucleon.
    • - p A --> J/PSI... 200 GeV
      DSIG/DPT v EKIN/A (1)(Location: T 4... Nucleus,U,Cu)
      DSIG/DPT v M (2)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... Nucleus,U,Cu)
    • - p A --> MU... 200 GeV
      DSIG/DPT v EKIN/A (1)(Location: T 4... Nucleus,U,Cu)
      DSIG/DPT v M (2)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... Nucleus,U,Cu)
  • Abreu et al. NP A566(1994)77C [R] - 2813688
    J / psi, psi-prime and muon pair production in p - W and S - U collisions
    • - p WT --> J/PSI... 200 GeV
      N v COS (1)(THE NEUTRAL TRANSVERSE ENERGY PRODUCED IN THE COLLISION > 15 GEV... -)
    • - p WT --> J/PSI... 200 GeV
      SIG/SIG v COS (2)(THE NEUTRAL TRANSVERSE ENERGY PRODUCED IN THE COLLISION > 15 GEV... -)
  • Abreu et al. PL B444(1998)516 [R] - 3877493
    Charmonia production in 450-GeV/c proton induced reactions
    • - p A --> J/PSI... 450 GeV
      SIG v RE (4)(The J/PSI cross sections per nucleon, times the BR to di-muons, obtained by divi... Nucleus,C,Al,Cu,Wt)
      SIG v RE (3)(The PSI(3685) absolute cross sections, times the BR to di-muons.... Nucleus,C,Al,Cu,Wt)
      SIG v RE (2)(The J/PSI absolute cross sections, times the BR to di-muons.... Nucleus,C,Al,Cu,Wt)
      SIG v YN (1)(The ratio of the production cross sections, in the di-muon channel. Note that th... Nucleus,C,Al,Cu,Wt)
    • - p A --> PSI... 450 GeV
      SIG v RE (4)(The J/PSI cross sections per nucleon, times the BR to di-muons, obtained by divi... Nucleus,C,Al,Cu,Wt)
      SIG v RE (3)(The PSI(3685) absolute cross sections, times the BR to di-muons.... Nucleus,C,Al,Cu,Wt)
      SIG v RE (2)(The J/PSI absolute cross sections, times the BR to di-muons.... Nucleus,C,Al,Cu,Wt)
      SIG v YN (1)(The ratio of the production cross sections, in the di-muon channel. Note that th... Nucleus,C,Al,Cu,Wt)
    • - p A --> J/PSI... 450 GeV
      POWER v PLAB (5)(Cross sections is fitted to SIG0*A**POWER... Nucleus,C,Al,Cu,Wt)
  • Abreu et al. PL B466(1999)408 [R] - 4173252
    J / psi and psi-prime production in p, O and S induced reactions at SPS energies
    • - p A --> J/PSI... 200,450 GeV
      POWER v PLAB (1)(Results of fitting the 200 and 450 GeV J/PSI data separately with a power law pa... Al,C,Cu,Deut,P,U)
    • - p A --> J/PSI... 200,450 GeV
      SIG v YN (6)(The PSI(3658) cross sections per nucleon-nucleon collisions as estimated from th... Al,C,Cu,Deut,P,U)
      SIG v YN (4)(The ratio between the PSI(3685) and the J/PSI production cross section, times th... Al,C,Cu,Deut,P,U)
      SIG v YN (3)(The ratio between the PSI(3685) and the J/PSI production cross section, times th... Al,C,Cu,Deut,P,U)
      SIG v RE (2)(The J/PSI cross sections per nucleon (times the BR to di-muons) rescaled to 200 ... Al,C,Cu,Deut,P,U)
    • - p A --> PSI... 200,450 GeV
      SIG v YN (6)(The PSI(3658) cross sections per nucleon-nucleon collisions as estimated from th... Al,C,Cu,Deut,P,U)
      SIG v YN (4)(The ratio between the PSI(3685) and the J/PSI production cross section, times th... Al,C,Cu,Deut,P,U)
      SIG v YN (3)(The ratio between the PSI(3685) and the J/PSI production cross section, times th... Al,C,Cu,Deut,P,U)
      SIG v RE (2)(The J/PSI cross sections per nucleon (times the BR to di-muons) rescaled to 200 ... Al,C,Cu,Deut,P,U)
  • Baglin et al. NP A566(1994)371C [R] - 4070976
    psi-Prime and J / psi production in p W, p U and S U interactions at 200-GeV/nucleon
    • - p A --> J/PSI... 200 GeV
      SIG v E (1)(Location: T 2... Nucleus,Wt)
      SIG v MEAN(ET) (2)(Location: T 2... Nucleus,Wt)
    • - p A --> PSI... 200 GeV
      SIG v E (1)(Location: T 2... Nucleus,Wt)
      SIG v MEAN(ET) (2)(Location: T 2... Nucleus,Wt)
  • Guichard et al. NP A525(1991)469C [R] - 3799352
    Transverse momentum of dimuons production in p U, O U and S U collisions at 200-GeV/nucleon
    • - p A --> MU... 200 GeV
      PT v M (1)(Location: T 1... U)
      PT v M (3)(Location: T 1... U)
    • - p A --> J/PSI... 200 GeV
      PT v M (1)(Location: T 1... U)
      PT v M (3)(Location: T 1... U)
    • - p A --> MU... 200 GeV
      PT**2 v M (2)(Location: T 1... U)
      PT**2 v M (4)(Location: T 1... U)
    • - p A --> J/PSI... 200 GeV
      PT**2 v M (2)(Location: T 1... U)
      PT**2 v M (4)(Location: T 1... U)
  • Baglin et al. PL B270(1991)105 [R] - 3506665
    J / psi and muon pair cross-sections in proton nucleus and nucleus-nucleus collisions at 200-GeV per nucleon
NA50
  • Abreu et al. EPJ C14(2000)443 [R] - 4328744
    Dimuon and charm production in nucleus-nucleus collisions at the CERN SPS
    • - p A --> MU... 158 GeV
  • Abreu et al. PL B410(1997)337 [R] - 4621760
    Anomalous J / psi suppression in Pb - Pb interactions at 158 GeV/c per nucleon
    • - P A --> J/PSI... 158 GeV
      SIG/SIG v ET (2)(Different data are rescaled at 200 GeV... Nucleon)
  • Alessandro et al. PL B553(2003)167 [R] - 5463696
    Charmonia and Drell-Yan production in proton-nucleus collisions at the CERN SPS
    • - p A --> J/PSI... 450 GeV
      SIG v RE (1)(The J/PSI production cross section times the branching ratio to MU+ MU- pernucle... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (2)(The PSI(3685) production cross section times the branching ratio to MU+ MU-per n... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (3)(The Drell Yan cross section, divided by the mass number A, and multiplied by the... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v NUCLEUS (4)(Ratio of charmonium to Drell Yan cross section. The third column shows the J/PSI... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v NUCLEUS (5)(Ratio between the PSI(3685) and J/PSI cross section.... Nucleus,Be,Al,Cu,Ag,Wt)
    • - p A --> PSI... 450 GeV
      SIG v RE (1)(The J/PSI production cross section times the branching ratio to MU+ MU- pernucle... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (2)(The PSI(3685) production cross section times the branching ratio to MU+ MU-per n... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (3)(The Drell Yan cross section, divided by the mass number A, and multiplied by the... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v NUCLEUS (4)(Ratio of charmonium to Drell Yan cross section. The third column shows the J/PSI... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v NUCLEUS (5)(Ratio between the PSI(3685) and J/PSI cross section.... Nucleus,Be,Al,Cu,Ag,Wt)
    • - p A --> MU... 450 GeV
      SIG v RE (1)(The J/PSI production cross section times the branching ratio to MU+ MU- pernucle... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (2)(The PSI(3685) production cross section times the branching ratio to MU+ MU-per n... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (3)(The Drell Yan cross section, divided by the mass number A, and multiplied by the... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v NUCLEUS (4)(Ratio of charmonium to Drell Yan cross section. The third column shows the J/PSI... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v NUCLEUS (5)(Ratio between the PSI(3685) and J/PSI cross section.... Nucleus,Be,Al,Cu,Ag,Wt)
  • Alessandro et al. EPJ C33(2004)31 [R] - 5688272
    Charmonium production and nuclear absorption in p A interactions at 450-GeV
    • - p A --> J/PSI... 450 GeV
      SIG v XL (5)(J/PSI production cross section times the di-muon branching ratio for the CUtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (6)(J/PSI production cross section times the di-muon branching ratio for the AGtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (7)(J/PSI production cross section times the di-muon branching ratio for the WTtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (8)(PSI(3685) production cross section times the di-muon branching ratio for the BE ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (9)(PSI(3685) production cross section times the di-muon branching ratio for the AL ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (4)(J/PSI production cross section times the di-muon branching ratio for the ALtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (3)(J/PSI production cross section times the di-muon branching ratio for the BEtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (2)(The PSI(3685) production cross sections, per target nucleon, times the di-muon b... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (10)(PSI(3685) production cross section times the di-muon branching ratio for the CU ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (1)(The J/PSI production cross sections, per target nucleon, times the di-muon branc... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (11)(PSI(3685) production cross section times the di-muon branching ratio for the AG ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (12)(PSI(3685) production cross section times the di-muon branching ratio for the WT ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v NUCLEUS (13)(The PSI(3685) to J/PSI cross section ratios.... Nucleus,Be,Al,Cu,Ag,Wt)
    • - p A --> PSI... 450 GeV
      SIG v XL (5)(J/PSI production cross section times the di-muon branching ratio for the CUtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (6)(J/PSI production cross section times the di-muon branching ratio for the AGtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (7)(J/PSI production cross section times the di-muon branching ratio for the WTtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (8)(PSI(3685) production cross section times the di-muon branching ratio for the BE ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (9)(PSI(3685) production cross section times the di-muon branching ratio for the AL ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (4)(J/PSI production cross section times the di-muon branching ratio for the ALtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (3)(J/PSI production cross section times the di-muon branching ratio for the BEtarge... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (2)(The PSI(3685) production cross sections, per target nucleon, times the di-muon b... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (10)(PSI(3685) production cross section times the di-muon branching ratio for the CU ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (1)(The J/PSI production cross sections, per target nucleon, times the di-muon branc... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (11)(PSI(3685) production cross section times the di-muon branching ratio for the AG ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v XL (12)(PSI(3685) production cross section times the di-muon branching ratio for the WT ... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v NUCLEUS (13)(The PSI(3685) to J/PSI cross section ratios.... Nucleus,Be,Al,Cu,Ag,Wt)
  • Alessandro et al. PL B635(2006)260 [R] - 6567150
    Bottomonium and Drell-Yan production in p-A collisions at 450- GeV
    • - p A --> UPSI... 450 GeV
      SIG v RE (1)(Drell-Yann (for the mass region MMUMU>6GeV/c**2) and bottomonium cross sectio... Be,Al,Cu,Ag,Wt)
    • - p A --> UPSI... 450 GeV
      PT v RE (2)(Mean pT and Mean PT**2 for Drell-Yann (4.5<MMUMU<8 GeV/c**2) Errors for Dr... Be,Al,Cu,Ag,Wt)
    • - p A --> UPSI... 450 GeV
      POWER(N v Ecm (3)(ALPHA parameter... Be,Al,Cu,Ag,Wt)
  • Alessandro et al. EPJ C48(2006)329 [R] - 7006500
    J/psi and psi-prime production and their normal nuclear absorption in proton-nucleus collisions at 400-GeV
    • - p A --> J/PSI,PSI... 450 GeV
      SIG v RE (1)(Production cross sections, per taregt nucleon for J/PSI and PSI(3685) and for Dr... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v RE (2)(Ratios of J/PSI, PSI(3685) and Drel Yann production cross sections, and for Dre... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v PLAB (3)(Absorption cross-section obtained with Glauber fits results only from this analy... Nucleus,Be,Al,Cu,Ag,Wt)
      SIG v PLAB (4)(Absorption cross-section obtained with Glauber fits results combined with previo... Nucleus,Be,Al,Cu,Ag,Wt)