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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 NUCLEUS_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.
PHENIX - STAR - NA34-3 - NA38 - NA50 - NA60 - ALICE - ATLAS -

PHENIX

  • Adler et al. PR C69(2004)014901 [R] - 5562031
    J / psi production in Au Au collisions at s(NN)**(1/2) = 200-GeV at the Relativistic Heavy Ion Collider
    • - Au Au --> J/PSI... 200 GeV
      DN/DETARAP v CENTRALITY (1)(Measured invariant differential yield at mid-rapidity of J/PSI, as a function of... -)
      DN/DETARAP v CENTRALITY (2)(Measured differential yield of J/PSI per binary collisions,at mid rapidity, as a... -)
  • Adare et al. PRL 98(2007)232301 [R] - 6978410
    J/psi Production vs Centrality, Transverse Momentum, and Rapidity in Au+Au Collisions at s(NN)**(1/2) = 200-GeV
    • - Au Au --> J/PSI... 200 GeV
      RAA v CENTRALITY (13)(Ratio of nuclear modification factors RAA(forward rapidity)/RAA(mid rapidity), v... -)
      RAA v CENTRALITY (12)(The number of participants Npart and the nuclear modification factor Raa versus ... -)
      RAA v CENTRALITY (11)(The number of participants Npart and the nuclear modification factor Raa versus ... -)
      RAA v YRAP (10)(Nuclear modification factor Raa versus rapidity for 0-20%, 20-40%, 40-60%, 60-92... -)
      RAA v YRAP (9)(Nuclear modification factor Raa versus rapidity for 0-20%, 20-40%, 40-60%, 60-92... -)
      RAA v PT (8)(Nuclear modification factor Raa versus transverse momentum for 0-20%, 20-40%, 40... -)
      RAA v PT (7)(Nuclear modification factor Raa versus transverse momentum for 0-20%, 20-40%, 40... -)
    • - Au Au --> J/PSI... 200 GeV
      DN/DPT/DYRAP v YRAP (6)(J/PSI invariant yield versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrali... -)
      DN/DPT/DYRAP v YRAP (5)(J/PSI invariant yield versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrali... -)
      DN/DPT/DYRAP v PT (2)(J/PSI invariant yield versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-9... -)
      DN/DPT/DYRAP v PT (1)(J/PSI invariant yield versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-9... -)
    • - Au Au --> J/PSI... 200 GeV
      PT**2 v CENTRALITY (3)(Mean PT^2 values for different bins of centrality, at mid rapidities :-0.35<y... -)
  • Adare et al. PRL 98(2007)232002 [R] - 6977820
    $J/\\psi$ production versus transverse momentum and rapidity in $p^+ p$ collisions at $\\sqrt{s}$ = 200-GeV
    • - Au Au --> J/PSI... 200 GeV
      PT**2 v Ecm (4)(Mean PT^2 value at forward rapidities : absolute value of y belongs to [1.2;2.2]... -)
      PT**2 v Ecm (3)(Mean PT^2 value at mid rapidities : -0.35<y<0.35 The mean PT is obtained w... -)
  • Adare et al. PRL 101(2008)122301 [R] - 7601360
    J/psi Production in s(NN)**(1/2) = 200-GeV Cu+Cu Collisions
    • - Cu Cu --> J/PSI... 200 GeV
      RAA v PT (11)(Nuclear modification factor RAA versus transverse momentum PT at mid rapidity : ... -)
      RAA v PT (12)(Nuclear modification factor RAA versus transverse momentum PT at forward rapidit... -)
      RAA v YRAP (13)(Nuclear modification factor RAA versus rapidity, for the 0-20% most central even... -)
      RAA v N (14)(Nuclear modification factor RAA versus number of participants, at mid rapidity :... -)
    • - Cu Cu --> J/PSI... 200 GeV
      DN/DPT/DYRAP v PT (8)(J/PSI yield versus transverse momentum PT, at forward rapidity : absolute value... -)
      DN/DPT/DYRAP v PT (7)(J/PSI yield versus transverse momentum PT, at forward rapidity : absolute value... -)
      DN/DPT/DYRAP v PT (6)(J/PSI yield versus transverse momentum PT, at forward rapidity : absolute value... -)
      DN/DPT/DYRAP v PT (5)(J/PSI yield versus transverse momentum PT, at forward rapidity : absolute value... -)
      DN/DPT/DYRAP v PT (4)(J/PSI yield versus transverse momentum PT, at mid rapidity : -0.35<y<0.35... -)
      DN/DPT/DYRAP v PT (3)(J/PSI yield versus transverse momentum PT, at mid rapidity : -0.35<y<0.35... -)
      DN/DPT/DYRAP v PT (2)(J/PSI yield versus transverse momentum PT, at mid rapidity : -0.35<y<0.35... -)
      DN/DPT/DYRAP v PT (1)(J/PSI yield versus transverse momentum PT, at mid rapidity : -0.35<y<0.35... -)
    • - Cu Cu --> J/PSI... 200 GeV
      PT**2 v N (10)(Mean PT^2 versus Npart, number of participants, at forward rapidity : absolute v... -)
  • Afanasiev et al. PL B679(2009)321 [R] - 8204152
    Photoproduction of J/psi and of high mass e+e- in ultra-peripheral Au+Au collisions at s**(1/2) = 200-GeV
    • - Au Au --> J/PSI... 200 GeV
      N v Ecm (1)(J/PSI N for ultra peripheral Au+Au reactions. The values has been obtained from ... -)
      N v Ecm (2)(e+e- pairs N in ultra peripherals Au + Au reactions. The values has been obtaine... -)
    • - Au Au --> J/PSI... 200 GeV
      SIG v Ecm (3)(J/PSI production cross section at mid rapidity for ultra peripheral Au+Au reacti... -)
      SIG v Ecm (4)(e+e- production cross section at mid rapidity for ultra peripheral Au+Au reactio... -)
    • - Au Au --> E... 200 GeV
      N v Ecm (1)(J/PSI N for ultra peripheral Au+Au reactions. The values has been obtained from ... -)
      N v Ecm (2)(e+e- pairs N in ultra peripherals Au + Au reactions. The values has been obtaine... -)
    • - Au Au --> E... 200 GeV
      SIG v Ecm (3)(J/PSI production cross section at mid rapidity for ultra peripheral Au+Au reacti... -)
      SIG v Ecm (4)(e+e- production cross section at mid rapidity for ultra peripheral Au+Au reactio... -)
  • Adler et al. PRL 94(2005)082301 [R] - 6006019
    Centrality dependence of charm production from single electrons measurement in Au + Au collisions at s(NN)**(1/2) = 200-GeV
    • - Au Au --> CHARM... 200 GeV
      POWER v Ecm (2)(Value of the Alpha power as used in a fit of dN/dy versus Ncoll, of the form A*N... -)
      POWER v Ecm (1)(Value of the Alpha power as used in a fit of dN/dy versus Ncoll of the form A*Nc... -)
    • - Au Au --> B... 200 GeV
      POWER v Ecm (2)(Value of the Alpha power as used in a fit of dN/dy versus Ncoll, of the form A*N... -)
      POWER v Ecm (1)(Value of the Alpha power as used in a fit of dN/dy versus Ncoll of the form A*Nc... -)
    • - Au Au --> CHARM... 200 GeV
      DN/DPT/DYRAP v PT (8)(Spectra in transverse momentum of electrons created in open heavy flavor decays,... -)
      DN/DPT/DYRAP v PT (7)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
      DN/DPT/DYRAP v PT (6)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
      DN/DPT/DYRAP v PT (5)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
      DN/DPT/DYRAP v PT (4)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
      DN/DPT/DYRAP v PT (3)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
    • - Au Au --> B... 200 GeV
      DN/DPT/DYRAP v PT (8)(Spectra in transverse momentum of electrons created in open heavy flavor decays,... -)
      DN/DPT/DYRAP v PT (7)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
      DN/DPT/DYRAP v PT (6)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
      DN/DPT/DYRAP v PT (5)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
      DN/DPT/DYRAP v PT (4)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
      DN/DPT/DYRAP v PT (3)(Spectrum in transverse momentum of electrons created in open heavy flavor decays... -)
    • - Au Au --> CHARM... 200 GeV
      N v Ecm (12)(Number of collisions for minimum bias events There are only systematic errors du... -)
      N v CENTRALITY (11)(Number of collisions as a fonction of centrality There are only systematic error... -)
    • - Au Au --> B... 200 GeV
      N v Ecm (12)(Number of collisions for minimum bias events There are only systematic errors du... -)
      N v CENTRALITY (11)(Number of collisions as a fonction of centrality There are only systematic error... -)
    • - Au Au --> CHARM... 200 GeV
      SIG v Ecm (14)(Nuclear overlap function TAA for minimum bias events The axis is labelled with 1... -)
      SIG v PT (13)(Nuclear overlap function TAA as a function of centrality The axis is labelled wi... -)
      SIG v Ecm (18)(Total charm cross section scaled by the number of collisions, for minimum bias e... -)
      SIG v CENTRALITY (17)(Total charm cross section scaled by the number of collisions, as a function of c... -)
    • - Au Au --> B... 200 GeV
      SIG v Ecm (14)(Nuclear overlap function TAA for minimum bias events The axis is labelled with 1... -)
      SIG v PT (13)(Nuclear overlap function TAA as a function of centrality The axis is labelled wi... -)
      SIG v Ecm (18)(Total charm cross section scaled by the number of collisions, for minimum bias e... -)
      SIG v CENTRALITY (17)(Total charm cross section scaled by the number of collisions, as a function of c... -)
    • - Au Au --> CHARM... 200 GeV
      DSIG/DYRAP v CENTRALITY (15)(Differential charm cross section scaled by the number of collisions, at mid rapi... -)
      DSIG/DYRAP v Ecm (16)(Differential charm cross section scaled by the number of collisions, at mid rapi... -)
  • Adler et al. PRL 96(2006)032301 [R] - 6398847
    Nuclear modification of electron spectra and implications for heavy quark energy loss in Au+Au collisions at s(NN)**(1/2) - 200-GeV
    • - Au Au --> CHARM... 200 GeV
      DN/DPT/DYRAP v PT (2)(Non photonic electrons invariant yield versus PT for different ranges of central... -)
      DN/DPT/DYRAP v PT (1)(Inclusive and non photonic electrons invariant yield versus PT, for minimum bias... -)
    • - Au Au --> B... 200 GeV
      DN/DPT/DYRAP v PT (2)(Non photonic electrons invariant yield versus PT for different ranges of central... -)
      DN/DPT/DYRAP v PT (1)(Inclusive and non photonic electrons invariant yield versus PT, for minimum bias... -)
    • - Au Au --> E... 200 GeV
      DN/DPT/DYRAP v PT (2)(Non photonic electrons invariant yield versus PT for different ranges of central... -)
      DN/DPT/DYRAP v PT (1)(Inclusive and non photonic electrons invariant yield versus PT, for minimum bias... -)
    • - Au Au --> CHARM... 200 GeV
      RAA v PT (5)(Nuclear modification factor as a function of PT, for 20-40% central reactions N... -)
      RAA v PT (3)(Nuclear modification factor as a function of PT, for 0-10% central reactions No... -)
      RAA v PT (4)(Nuclear modification factor as a function of PT, for 10-20% central reactions N... -)
      RAA v PT (6)(Nuclear modification factor as a function of PT, for 40-60% central reactions N... -)
    • - Au Au --> B... 200 GeV
      RAA v PT (5)(Nuclear modification factor as a function of PT, for 20-40% central reactions N... -)
      RAA v PT (3)(Nuclear modification factor as a function of PT, for 0-10% central reactions No... -)
      RAA v PT (4)(Nuclear modification factor as a function of PT, for 10-20% central reactions N... -)
      RAA v PT (6)(Nuclear modification factor as a function of PT, for 40-60% central reactions N... -)
STAR
  • Abelev et al. PR C80(2009)041902 [R] - 8228655
    J/psi production at high transverse momentum in p+p and Cu+Cu collisions at s(NN)**1/2 = 200GeV
    • - CU CU --> J/PSI... 200 GeV
      D2N/DYRAP/DPT v PT (2)(J/psi transverse momentum distribution in sqrt(s)... -)
      D2N/DYRAP/DPT v PT (3)(J/psi transverse momentum distribution in sqrt(s)... -)
    • - CU CU --> J/PSI... 200 GeV
      RAA v PT (5)(J/psi nuclear modification factor RAA from sqrt(s)... -)
      RAA v PT (6)(J/psi nuclear modification factor RAA from sqrt(s)... -)
  • Abelev et al. PRL 98(2007)192301 [R] - 6797547
    Erratum: Transverse momentum and centrality dependence of high-\\pt\\ non-photonic electron suppression in Au+Au collisions at \\sqrtsNN\\ = 200 GeV
    • - Au Au --> CHARM,B... 200 GeV
      RAA v PT (7)(Nuclear modification factor for non-photonic electrons in AU+AU reactions in the... -)
    • - Au Au --> CHARM,B... 200 GeV
      DN/DPT/DETARAP v PT (4)(Non photonic electron yield in AU+AU collisions versus PT, for a centrality rang... -)
      DN/DPT/DETARAP v PT (5)(Non photonic electron yield in AU+AU collisions versus PT, for a centrality rang... -)
      DN/DPT/DETARAP v PT (3)(Non photonic electron yield in AU+AU collisions versus PT, for a centrality rang... -)
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
    • - S WT --> MU... 200 GeV
      N v M (2)(Location: T 2... -)
      N v M (4)(Location: T 3... -)
      N v M (6)(Location: T 4... -)
      N v M (8)(Location: T 6... -)
NA38
  • Baglin et al. PL 220B(1989)471 [R] - 1807102
    THE PRODUCTION OF J / psi IN 200-GeV/A OXYGEN - URANIUM INTERACTIONS
    • - NUCLEUS NUCLEUS --> J/PSI... 200 GeV
  • Baglin et al. PL 251B(1990)465 [R] - 2379228
    Transverse momentum of J / psi produced in oxygen uranium collisions at 200-GeV per nucleon.
    • - O16 U --> J/PSI... 200 GeV
    • - O16 U --> MU... 200 GeV
    • - O16 U --> J/PSI... 200 GeV
      PT v ET (3)(D(SIG)/D(PT) is parameterized as PT*exp(-SLOPE*PT**CONST)... -)
      PT v ET (4)(D(SIG)/D(PT) is parameterized as PT*exp(-SLOPE*PT**CONST)... -)
    • - O16 U --> MU... 200 GeV
      PT v ET (3)(D(SIG)/D(PT) is parameterized as PT*exp(-SLOPE*PT**CONST)... -)
      PT v ET (4)(D(SIG)/D(PT) is parameterized as PT*exp(-SLOPE*PT**CONST)... -)
  • 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.
    • - O16 A --> J/PSI... 200 GeV
      DSIG/DPT v EKIN/A (1)(Location: T 4... Nucleus,Cu,U)
      DSIG/DPT v M (2)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... Nucleus,Cu,U)
      DSIG/DPT v ET (3)(Location: T 4... Nucleus,Cu,U)
      DSIG/DPT v ET (4)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... Nucleus,Cu,U)
      DSIG/DPT v ET (5)(Location: T 4... Nucleus,Cu,U)
      DSIG/DPT v ET (6)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... Nucleus,Cu,U)
    • - O16 A --> MU... 200 GeV
      DSIG/DPT v EKIN/A (1)(Location: T 4... Nucleus,Cu,U)
      DSIG/DPT v M (2)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... Nucleus,Cu,U)
      DSIG/DPT v ET (3)(Location: T 4... Nucleus,Cu,U)
      DSIG/DPT v ET (4)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... Nucleus,Cu,U)
      DSIG/DPT v ET (5)(Location: T 4... Nucleus,Cu,U)
      DSIG/DPT v ET (6)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... Nucleus,Cu,U)
    • - S32 A --> J/PSI... 200 GeV
      DSIG/DPT v EKIN/A (1)(Location: T 4... U)
      DSIG/DPT v M (2)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... U)
      DSIG/DPT v ET (7)(Location: T 4... U)
      DSIG/DPT v ET (8)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... U)
    • - S32 A --> MU... 200 GeV
      DSIG/DPT v EKIN/A (1)(Location: T 4... U)
      DSIG/DPT v M (2)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... U)
      DSIG/DPT v ET (7)(Location: T 4... U)
      DSIG/DPT v ET (8)(CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS ... U)
  • Abreu et al. NP A566(1994)77C [R] - 2813688
    J / psi, psi-prime and muon pair production in p - W and S - U collisions
    • - S U --> J/PSI... 200 GeV
      SIG/SIG v COS (2)(THE NEUTRAL TRANSVERSE ENERGY PRODUCED IN THE COLLISION > 15 GEV... -)
      SIG/SIG v ET (3)(THE NEUTRAL TRANSVERSE ENERGY PRODUCED IN THE COLLISION > 15 GEV... -)
    • - S U --> J/PSI... 200 GeV
      SIG v COS (4)(THE NEUTRAL TRANSVERSE ENERGY PRODUCED IN THE COLLISION > 15 GEV... -)
  • Abreu et al. PL B423(1998)208 [R] - 3705668
    Transverse momentum of J / psi, psi-prime and mass continuum muon pairs produced in S-32 U collisions at 200-GeV/c per nucleon
    • - S32 U --> MU... 200 GeV
      PT v ET (1)(Location: T 2... -)
      PT v ET (2)(Location: T 3... -)
    • - S32 U --> J/PSI... 200 GeV
      PT v ET (1)(Location: T 2... -)
      PT v ET (2)(Location: T 3... -)
    • - S32 U --> PSI... 200 GeV
      PT v ET (1)(Location: T 2... -)
      PT v ET (2)(Location: T 3... -)
    • - S32 U --> J/PSI... 200 GeV
      MT v ET (3)(Location: T 4... -)
    • - S32 U --> J/PSI... 200 GeV
      DN/DPT v PT (4)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (5)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (6)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (7)(Unfolded distribution. Center of the PT bin is given... -)
    • - S32 U --> PSI... 200 GeV
      DN/DPT v PT (4)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (5)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (6)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (7)(Unfolded distribution. Center of the PT bin is given... -)
    • - S32 U --> MU... 200 GeV
      DN/DPT v PT (4)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (5)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (6)(Unfolded distribution. Center of the PT bin is given... -)
      DN/DPT v PT (7)(Unfolded distribution. Center of the PT bin is given... -)
    • - S32 U --> J/PSI... 200 GeV
      DN/DMT v MT (8)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (9)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (10)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (11)(Unfolded distribution. Center of the (MT-M) bin is given... -)
    • - S32 U --> PSI... 200 GeV
      DN/DMT v MT (8)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (9)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (10)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (11)(Unfolded distribution. Center of the (MT-M) bin is given... -)
    • - S32 U --> MU... 200 GeV
      DN/DMT v MT (8)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (9)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (10)(Unfolded distribution. Center of the (MT-M) bin is given... -)
      DN/DMT v MT (11)(Unfolded distribution. Center of the (MT-M) bin is given... -)
  • Abreu et al. PL B449(1998)128 [R] - 3939103
    J / psi, psi-prime and Drell-Yan production in S U interactions at 200-GeV per nucleon
    • - S U --> J/PSI... 200 GeV
      SIG v PLAB/A (1)(Cross sections (times decay BR into di-muons) and ratios.... -)
      SIG v ET (2)(Centrality dependence of the rations of J/PSI/DY and PSI(3685)/J/PSI production... -)
    • - S U --> PSI... 200 GeV
      SIG v PLAB/A (1)(Cross sections (times decay BR into di-muons) and ratios.... -)
      SIG v ET (2)(Centrality dependence of the rations of J/PSI/DY and PSI(3685)/J/PSI production... -)
  • 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
    • - O 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... Cu,U)
    • - S 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... U)
    • - O A --> J/PSI... 200,450 GeV
      SIG v RE (2)(The J/PSI cross sections per nucleon (times the BR to di-muons) rescaled to 200 ... Cu,U)
    • - S A --> J/PSI... 200,450 GeV
      SIG v RE (2)(The J/PSI cross sections per nucleon (times the BR to di-muons) rescaled to 200 ... U)
      SIG v YN (6)(The PSI(3658) cross sections per nucleon-nucleon collisions as estimated from th... U)
    • - S A --> PSI... 200,450 GeV
      SIG v RE (2)(The J/PSI cross sections per nucleon (times the BR to di-muons) rescaled to 200 ... U)
      SIG v YN (6)(The PSI(3658) cross sections per nucleon-nucleon collisions as estimated from th... 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
  • 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
    • - S32 A --> MU... 200 GeV
      PT v M (1)(Location: T 1... U)
      PT v M (3)(Location: T 1... U)
    • - O16 A --> MU... 200 GeV
      PT v M (1)(Location: T 1... U)
      PT v M (3)(Location: T 1... U)
    • - S32 A --> J/PSI... 200 GeV
      PT v M (1)(Location: T 1... U)
      PT v M (3)(Location: T 1... U)
    • - O16 A --> J/PSI... 200 GeV
      PT v M (1)(Location: T 1... U)
      PT v M (3)(Location: T 1... U)
    • - S32 A --> MU... 200 GeV
      PT**2 v M (2)(Location: T 1... U)
      PT**2 v M (4)(Location: T 1... U)
    • - O16 A --> MU... 200 GeV
      PT**2 v M (2)(Location: T 1... U)
      PT**2 v M (4)(Location: T 1... U)
    • - S32 A --> J/PSI... 200 GeV
      PT**2 v M (2)(Location: T 1... U)
      PT**2 v M (4)(Location: T 1... U)
    • - O16 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
    • - Nucleus A --> J/PSI... 200 GeV
      POWER v PLAB (1)(Cross sections fitted with SIG0*(A(P=1)*A(P=2))** ALPHA. ALPHA is coded here as ... Nucleus)
      POWER v M (2)(Cross sections fitted with SIG0*(A(P=1)*A(P=2))** ALPHA. ALPHA is coded here as ... Nucleus)
    • - Nucleus A --> J/PSI... 200 GeV
      SIG v PLAB (1)(Cross sections fitted with SIG0*(A(P=1)*A(P=2))** ALPHA. ALPHA is coded here as ... Nucleus)
      SIG v M (2)(Cross sections fitted with SIG0*(A(P=1)*A(P=2))** ALPHA. ALPHA is coded here as ... Nucleus)
      SIG v PLAB (3)(Location: T 4... Nucleus)
      SIG v PLAB (4)(Location: T 4... Nucleus)
    • - Nucleus A --> MU... 200 GeV
      POWER v PLAB (1)(Cross sections fitted with SIG0*(A(P=1)*A(P=2))** ALPHA. ALPHA is coded here as ... Nucleus)
      POWER v M (2)(Cross sections fitted with SIG0*(A(P=1)*A(P=2))** ALPHA. ALPHA is coded here as ... Nucleus)
    • - Nucleus A --> MU... 200 GeV
      SIG v PLAB (1)(Cross sections fitted with SIG0*(A(P=1)*A(P=2))** ALPHA. ALPHA is coded here as ... Nucleus)
      SIG v M (2)(Cross sections fitted with SIG0*(A(P=1)*A(P=2))** ALPHA. ALPHA is coded here as ... Nucleus)
      SIG v PLAB (3)(Location: T 4... Nucleus)
      SIG v PLAB (4)(Location: T 4... Nucleus)
NA50
  • Abreu et al. NP A638(1998)261 [R] - 3927334
    Charmonium production in Pb Pb interactions at 158-GeV/c per nucleon
    • - PB PB --> J/PSI... 158 GeV
      SIG/SIG v ET (1)(ET - neutral transverse energy in the electromagnetic calorimeter, etarap=1.1-2.... -)
    • - PB PB --> MU... 158 GeV
      SIG/SIG v ET (1)(ET - neutral transverse energy in the electromagnetic calorimeter, etarap=1.1-2.... -)
  • Abreu et al. NP A610(1996)404c [R] - 4019652
    Anomalous J / psi suppression in Pb + Pb collisions at 158-A-GeV/c
    • - PB PB --> J/PSI... 158 GeV
      SIG v P/A (1)(Location: P 411c... -)
      SIG v P/A (2)(Location: P 412c... -)
    • - PB PB --> MU... 158 GeV
      SIG v P/A (1)(Location: P 411c... -)
      SIG v P/A (2)(Location: P 412c... -)
  • Abreu et al. PL B450(1997)456 [R] - 4064372
    Observation of a threshold effect in the anomalous J/ psi suppression
  • Abreu et al. PL B477(2000)28 [R] - 4328736
    Evidence for deconfinement of quarks and gluons from the J / psi suppression pattern measured in Pb + Pb collisions at the CERN SPS
    • - PB PB --> J/PSI... 158 GeV
      SIG/SIG v ET (1)(SIG(J/PSI)/SIG(DY) as a function of ET with the standard analyses of 1996. DATA ... -)
      SIG/SIG v ET (2)(SIG(J/PSI)/SIG(DY) as a function of ET with the minium bias analyses of 1996. D... -)
      SIG/SIG v ET (3)(SIG(J/PSI)/SIG(DY) as a function of E(NAME=TRANSVERSE) with the minium bias ana... -)
  • Abreu et al. EPJ C14(2000)443 [R] - 4328744
    Dimuon and charm production in nucleus-nucleus collisions at the CERN SPS
    • - A A --> MU... 200 GeV
    • - A A --> MU... 158 GeV
  • Abreu et al. PL B499(2000)85 [R] - 4509412
    Transverse momentum distributions of J / psi, psi-prime, Drell-Yan and continuum dimuons produced in Pb Pb interactions at the SPS
    • - PB PB --> MU... 158 GeV
      PT v ET (4)(Mean values of PT and PT**2 calculated from the Drell-Yan distributions.... -)
      PT v ET (3)(Mean values of PT and PT**2 calculated from the PSI(3685) distributions.... -)
      PT v ET (2)(Mean values of PT and PT**2 calculated from the J/PSI distributions.... -)
      PT v ET (1)(Mean values of PT and PT**2 calculated from the IMR distributions.... -)
    • - PB PB --> J/PSI... 158 GeV
      PT v ET (4)(Mean values of PT and PT**2 calculated from the Drell-Yan distributions.... -)
      PT v ET (3)(Mean values of PT and PT**2 calculated from the PSI(3685) distributions.... -)
      PT v ET (2)(Mean values of PT and PT**2 calculated from the J/PSI distributions.... -)
      PT v ET (1)(Mean values of PT and PT**2 calculated from the IMR distributions.... -)
    • - PB PB --> PSI... 158 GeV
      PT v ET (4)(Mean values of PT and PT**2 calculated from the Drell-Yan distributions.... -)
      PT v ET (3)(Mean values of PT and PT**2 calculated from the PSI(3685) distributions.... -)
      PT v ET (2)(Mean values of PT and PT**2 calculated from the J/PSI distributions.... -)
      PT v ET (1)(Mean values of PT and PT**2 calculated from the IMR distributions.... -)
    • - PB PB --> J/PSI... 158 GeV
    • - PB PB --> MU... 158 GeV
      DN/DPT v PT (6)(PT distribution from the IMR distributions. Data extracted from jpg figures with... -)
      DN/DPT v PT (7)(PT distribution from the J/PSI distributions. Data extracted from jpg figures wi... -)
      DN/DPT v PT (8)(PT distribution from the PSI(3685) distributions. Data extracted from jpg figure... -)
      DN/DPT v PT (9)(PT distribution from the Drell-Yan distributions. Data exctracted from jpg figur... -)
    • - PB PB --> J/PSI... 158 GeV
      DN/DPT v PT (6)(PT distribution from the IMR distributions. Data extracted from jpg figures with... -)
      DN/DPT v PT (7)(PT distribution from the J/PSI distributions. Data extracted from jpg figures wi... -)
      DN/DPT v PT (8)(PT distribution from the PSI(3685) distributions. Data extracted from jpg figure... -)
      DN/DPT v PT (9)(PT distribution from the Drell-Yan distributions. Data exctracted from jpg figur... -)
    • - PB PB --> PSI... 158 GeV
      DN/DPT v PT (6)(PT distribution from the IMR distributions. Data extracted from jpg figures with... -)
      DN/DPT v PT (7)(PT distribution from the J/PSI distributions. Data extracted from jpg figures wi... -)
      DN/DPT v PT (8)(PT distribution from the PSI(3685) distributions. Data extracted from jpg figure... -)
      DN/DPT v PT (9)(PT distribution from the Drell-Yan distributions. Data exctracted from jpg figur... -)
  • Abreu et al. PL B410(1997)337 [R] - 4621760
    Anomalous J / psi suppression in Pb - Pb interactions at 158 GeV/c per nucleon
    • - PB PB --> J/PSI... 158 GeV
      SIG v YRAP (1)(The results from other experiments are also presented... -)
  • Abreu et al. PL B410(1997)327 [R] - 4621778
    J / psi and Drell-Yan cross-sections in Pb Pb interactions at 158 GeV/c per nucleon
  • Abreu et al. PL B521(2001)195 [R] - 4754441
    The Dependence of the anomalous J / psi suppression on the number of participant nucleons
    • - PB PB --> J/PSI... 158 GeV
      DN/DE v E (1)(Minimum Bias E(C=ZDC) spectrum. Data extracted from fig with g3data, statistical... -)
    • - PB PB --> J/PSI... 158 GeV
      N v E (2)(Number of participants as a function of E(C=ZDC) Data exctracted from fig with g... -)
    • - PB PB --> J/PSI... 158 GeV
      SIG/SIG v E (3)(SIG(J/PSI)/SIG(DY) as a function of E(C=ZDC) with the standard analyses of the 1... -)
      SIG/SIG v E (4)(SIG(J/PSI)/SIG(DY) as a function of E(C=ZDC) with the standard analyses of the 1... -)
      SIG/SIG v E (5)(SIG(J/PSI)/SIG(DY) as a function of E(C=ZDC) with the minimum biasanalyses of th... -)
      SIG/SIG v E (6)(SIG(J/PSI)/SIG(DY) as a function of E(C=ZDC) with the minimum biasanalyses of th... -)
  • Alessandro et al. EPJ C39(2005)335 [R] - 6076947
    A New measurement of J/psi suppression in Pb-Pb collisions at 158-GeV per nucleon
    • - PB PB --> J/PSI... 158 GeV
      CENTRALITY v ET (1)(Centrality classes based on the transverse energy measurement Errors are rms val... -)
      CENTRALITY v E (6)(Centrality classes based on the forward energy measurement errors are rms values... -)
      CENTRALITY v D (11)(Centrality classes based on the Charged particle multiplicity : DN/DYRAP at YRAP... -)
    • - PB PB --> J/PSI... 158 GeV
      SIG/SIG v ET (2)(Cross sections ratio J/PSI/Drell-Yan as a function of ET IN GEV obtained withthe... -)
      SIG/SIG v N (3)(Cross sections ratio J/PSI/Drell-Yan as a function of NPART obtained withthe ET ... -)
      SIG/SIG v CENTRALITY (4)(Cross sections ratio J/PSI/Drell-Yan as a function of CENTRALITY(NAME=b) obtaine... -)
      SIG/SIG v CENTRALITY (5)(Cross sections ratio J/PSI/Drell-Yan as a function of CENTRALITY(NAME=L) obtaine... -)
      SIG/SIG v E (7)(Cross sections ratio J/PSI/Drell-Yan as a function of E(NAME=ZDC) obtained witht... -)
      SIG/SIG v N (8)(Cross sections ratio J/PSI/Drell-Yan as a function of N(NAME=PART) obtained with... -)
      SIG/SIG v CENTRALITY (9)(Cross sections ratio J/PSI/Drell-Yan as a function of CENTRALITY(NAME=b) obtaine... -)
      SIG/SIG v CENTRALITY (10)(Cross sections ratio J/PSI/Drell-Yan as a function of CENTRALITY(NAME=L) obtaine... -)
      SIG/SIG v D (12)(Cross sections ratio J/PSI/Drell-Yan as a function of N(NAME=CH) obtained withth... -)
      SIG/SIG v N (13)(Cross sections ratio J/PSI/Drell-Yan as a function of N(NAME=PART) obtained with... -)
      SIG/SIG v CENTRALITY (14)(Cross sections ratio J/PSI/Drell-Yan as a function of CENTRALITY(NAME=b) obtaine... -)
      SIG/SIG v CENTRALITY (15)(Cross sections ratio J/PSI/Drell-Yan as a function of CENTRALITY(NAME=L) obtaine... -)
  • Alessandro et al. EPJ C49(2007)559 [R] - 7006519
    psi-prime production in Pb-Pb collisions at 158-GeV/nucleon
    • - PB PB --> J/PSI... 158 GeV
      SIG v PLAB (1)(Inclusive cross sections for PSI(3685) and J/PSI, multiplied by their Branching ... -)
      SIG v PLAB (2)(Inclusive cross sections for Drell Yan in the 4.2-7 GeV/c** mass range.... -)
    • - PB PB --> MU... 158 GeV
      SIG v PLAB (1)(Inclusive cross sections for PSI(3685) and J/PSI, multiplied by their Branching ... -)
      SIG v PLAB (2)(Inclusive cross sections for Drell Yan in the 4.2-7 GeV/c** mass range.... -)
    • - PB PB --> MU... 158 GeV
      SIG/SIG v ET (3)(Inclusive cross sections for PSI(3685) and J/PSI, multiplied by theirBransching ... -)
      SIG/SIG v CENTRALITY (5)(SIG(PSI(3685))/SIG(DY) as functions of the mean free path crossed by the CCBAR p... -)
      SIG/SIG v N (6)(SIG(PSI(3685))/SIG(DY) as functions of the number of participating nucleon... -)
      SIG/SIG v E (7)(SIG(PSI(3685))/SIG(DY) as functions of the energy density... -)
    • - PB PB --> PSI... 158 GeV
      SIG/SIG v ET (3)(Inclusive cross sections for PSI(3685) and J/PSI, multiplied by theirBransching ... -)
      SIG/SIG v CENTRALITY (5)(SIG(PSI(3685))/SIG(DY) as functions of the mean free path crossed by the CCBAR p... -)
      SIG/SIG v N (6)(SIG(PSI(3685))/SIG(DY) as functions of the number of participating nucleon... -)
      SIG/SIG v E (7)(SIG(PSI(3685))/SIG(DY) as functions of the energy density... -)
NA60
  • Arnaldi et al. PRL 99(2007)132302 [R] - 7555512
    J/psi production in indium-indium collisions at 158-GeV/nucleon
    • - IN IN --> J/PSI... 158 GeV
      SIG/SIG v E (1)(Values of the J/PSI production cross section, divided by the Drell-Yann cross se... -)
  • Arnaldi et al. EPJ C59(2009)607 [R] - 8024804
    Evidence for the production of thermal-like muon pairs with masses above 1-GeV/c**2 in 158-A-GeV Indium-Indium Collisions
    • - IN IN --> CHARM... 158 GeV
      SIG v Ecm (1)(Charm production cross section, calculated from the yield of muons pairs coming ... -)
ALICE
  • Aamodt et al. CERN-PH-EP-2012-012 - 9369562
    J/psi production at low transverse momentum in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV
    • - PB PB --> J/PSI... 2760 GeV
  • Aamodt et al. CERN-PH-EP-2012-069 - 9414827
    Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV
    • - PB PB --> D... 2760 GeV
  • Aamodt et al. CERN-PH-EP-2012-055 - 9420169
    Inclusive $J/\psi$ production in $pp$ collisions at $\sqrt{s} = 2.76$ TeV
    • - PB PB --> J/PSI... 2760 GeV
    • - PB PB --> J/PSI... 2760 GeV
    • - PB PB --> J/PSI... 2760 GeV
ATLAS
  • Aad et al. PL B697(2011)294 - 8919828
    Measurement of the centrality dependence of J/{\psi} yields and observation of Z production in lead-lead collisions with the ATLAS detector at the LHC
    • - PB PB --> J/PSI... 2760 GeV