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PHENIX QUARKONII data
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Data from the PHENIX Collaboration
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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.
- 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
- Adler et al. PRL 92(2004)051802
[R] - 5602254
$J/\\psi$ production from proton proton collisions at $\\sqrt{s}$ = 200-GeV
- - p p --> J/PSI... 200 GeV DSIG/DPT/DYRAP
| DSIG/DPT/DYRAP v PT (2) | | (Measured J/PSI distribution in PT for the mu+mu- channel. The value of B, the br... -) |
| DSIG/DPT/DYRAP v PT (1) | | (Measured J/PSI distribution in PT for the e+e- channel. The value of B, the bran... -) |
- - p p --> J/PSI... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v YRAP (3) | | (J/PSI distribution in rapidity. The data at rapidity = 0 is from the electron ar... -) |
- - p p --> J/PSI... 200 GeV PT
| PT v Ecm (4) | | (Mean PT value for J/PSI production. The mean PT is obtained with a phenomonologi... -) |
- - p p --> J/PSI... 200 GeV SIG
| SIG v Ecm (5) | | (Value of the total cross-section for J/PSI production. The total cross section i... -) |
- Adler et al. PRL 96(2006)012304
[R] - 6298885
J/psi production and nuclear effects for d+Au and p+p collisions at s(NN)**(1/2) = 200-GeV
- - p p --> J/PSI... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v YRAP (1) | | (J/PSI differential cross section in P+P reactions( times di-lepton branching rat... -) |
- - deut A --> J/PSI... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v YRAP (2) | | (J/PSI nuclear modification factor RDA,as a function of rapidity.... Au) |
- - p p --> J/PSI... 200 GeV SIG
| SIG v Ecm (3) | | (Total cross-section for J/PSI production in P P reactions. The total cross secti... -) |
- - deut A --> J/PSI... 200 GeV PT**2
| PT**2 v Ecm (4) | | (Mean PT^2 values at negative, null and positive XF for D+AU reaction The mean PT... Au) |
- - p p --> J/PSI... 200 GeV PT**2
| PT**2 v Ecm (5) | | (Mean PT^2 values at negative,null and positive XF for P+P reaction The mean PT i... -) |
- - deut A --> J/PSI... 200 GeV POWER
| POWER v PT (8) | | (PT dependance of the Alpha power for Xf ~ 0.09... Au) |
| POWER v PT (7) | | (PT dependance of the Alpha power for Xf ~ 0.... Au) |
| POWER v PT (6) | | (PT dependence of the Alpha power for Xf ~ -0.08.... Au) |
- - deut A --> J/PSI... 200 GeV RDA
| RDA v N (10) | | (Centrality dependance of the Nuclear modification factor for rapidity y=0.Centra... Au) |
| RDA v N (9) | | (Centrality dependance of the Nuclear modification factor for rapidity : y=-1.7. ... Au) |
- 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
| 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
| 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
| 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
- - p p --> J/PSI... 200 GeV DSIG/DPT/DYRAP
| DSIG/DPT/DYRAP v PT (2) | | (J/PSI differential cross section, times dilepton branching ratio, versus transve... -) |
| DSIG/DPT/DYRAP v PT (1) | | (J/PSI differential cross section, times dilepton branching ratio, versus transve... -) |
- - Au Au --> J/PSI... 200 GeV PT**2
| 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... -) |
- - p p --> J/PSI... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v YRAP (5) | | (J/PSI differential cross section times dilepton branching ratio versus rapidity... -) |
- - p p --> J/PSI... 200 GeV SIG
| SIG v Ecm (6) | | (Total cross-section for J/PSI production. The value of the total cross section h... -) |
- 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
| 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
| 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
| PT**2 v N (10) | | (Mean PT^2 versus Npart, number of participants, at forward rapidity : absolute v... -) |
- Adare et al. PR C77(2008)024912
[R] - 7541414
Cold Nuclear Matter Effects on J/Psi as Constrained by Deuteron-Gold Measurements at s(NN)**(1/2) = 200-GeV
- - deut A --> J/PSI... 200 GeV SIG
| SIG v YRAP (22) | | (Breakup cross section of c-c_bar pairs inside cold nuclear matter for different ... Au) |
| SIG v Ecm (21) | | (Breakup cross section of c-c_bar pairs inside cold nuclear matter, integrated ov... Au) |
| SIG v YRAP (20) | | (Breakup cross section of c-c_bar pairs inside cold nuclear matter for different ... Au) |
| SIG v Ecm (19) | | (Breakup cross section of c-c_bar pairs inside cold nuclear matter,integrated ove... Au) |
- - deut A --> J/PSI... 200 GeV D2N/DPT/DYRAP
| D2N/DPT/DYRAP v PT (5) | | (J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus PT at forward rapidity (1.2&... Au) |
| D2N/DPT/DYRAP v PT (4) | | (J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus PT at mid rapidity (-0.35<... Au) |
| D2N/DPT/DYRAP v PT (3) | | (J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus PT at backward rapidity (-2.... Au) |
| D2N/DPT/DYRAP v YRAP (2) | | (J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus rapidity in D+AU collisions,... Au) |
| D2N/DPT/DYRAP v YRAP (1) | | (J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus rapidity in D+AU collisions,... Au) |
- - deut A --> J/PSI... 200 GeV RDA
| RDA v CENTRALITY (16) | | (Nuclear modification factor versus centrality at forward rapidity (1.2<y<... Au) |
| RDA v CENTRALITY (15) | | (Nuclear modification factor versus centrality at mid rapidity (-0.35<y<0.... Au) |
| RDA v CENTRALITY (14) | | (Nuclear modification factor versus centrality at backward rapidity (-2.2<y&l... Au) |
| RDA v PT (13) | | (Nuclear modification factor versus PT at forward rapidity (1.2<y<2.2) in D... Au) |
| RDA v PT (12) | | (Nuclear modification factor versus PT at mid rapidity (-0.35<y<0.35) in D+... Au) |
| RDA v PT (11) | | (Nuclear modification factor versus PT at backward rapidity (-2.2<y<-1.2) i... Au) |
| RDA v YRAP (10) | | (Nuclear modification factor versus rapidity in D+AU collisions, over 5 bins of r... Au) |
| RDA v YRAP (9) | | (Nuclear modification factor versus rapidity in D+AU collisions, over 3 bins of r... Au) |
- 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
| N v Ecm (1) | | (J/PSI N for ultra peripheral Au+Au reactions. The values has been obtained from ... -) |
- - Au Au --> J/PSI... 200 GeV SIG
| SIG v Ecm (3) | | (J/PSI production cross section at mid rapidity for ultra peripheral Au+Au reacti... -) |
- - Au Au --> E... 200 GeV N
| 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
| 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
| 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
| 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
| 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
| 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
| 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
| 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
| 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
| 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... -) |
- - Au Au --> CHARM... 200 GeV DSIG/DYRAP
| 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
| 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
| 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
| DN/DPT/DYRAP v PT (1) | | (Inclusive and non photonic electrons invariant yield versus PT, for minimum bias... -) |
- - Au Au --> CHARM... 200 GeV RAA
| 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
| 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... -) |
- Adare et al. PRL 98(2007)172301
[R] - 6978398
Energy Loss and Flow of Heavy Quarks in Au+Au Collisions at s(NN)**(1/2) = 200-GeV
- - Au AU --> CHARM... 200 GeV D2N/DPT/DYRAP
| D2N/DPT/DYRAP v PT (6) | | (Invariant yield of electrons from heavy-flavor decays for minimum bias collision... -) |
| D2N/DPT/DYRAP v PT (5) | | (Invariant yield of electrons from heavy-flavor decays for 60-92% central collisi... -) |
| D2N/DPT/DYRAP v PT (4) | | (Invariant yield of electrons from heavy-flavor decays for 40-60% central collisi... -) |
| D2N/DPT/DYRAP v PT (3) | | (Invariant yield of electrons from heavy-flavor decays for 20-40% central collisi... -) |
| D2N/DPT/DYRAP v PT (2) | | (Invariant yield of electrons from heavy-flavor decays for 10-20% central collisi... -) |
| D2N/DPT/DYRAP v PT (1) | | (Invariant yield of electrons from heavy-flavor decays for 0-10% central collisio... -) |
- - Au AU --> B... 200 GeV D2N/DPT/DYRAP
| D2N/DPT/DYRAP v PT (6) | | (Invariant yield of electrons from heavy-flavor decays for minimum bias collision... -) |
| D2N/DPT/DYRAP v PT (5) | | (Invariant yield of electrons from heavy-flavor decays for 60-92% central collisi... -) |
| D2N/DPT/DYRAP v PT (4) | | (Invariant yield of electrons from heavy-flavor decays for 40-60% central collisi... -) |
| D2N/DPT/DYRAP v PT (3) | | (Invariant yield of electrons from heavy-flavor decays for 20-40% central collisi... -) |
| D2N/DPT/DYRAP v PT (2) | | (Invariant yield of electrons from heavy-flavor decays for 10-20% central collisi... -) |
| D2N/DPT/DYRAP v PT (1) | | (Invariant yield of electrons from heavy-flavor decays for 0-10% central collisio... -) |
- Adare et al. PRL 97(2006)252002
[R] - 6896430
Measurement of high-p(T) single electrons from heavy-flavor decays in p+p collisions at s**(1/2) = 200-GeV
- - p p --> CHARM... 200 GeV E*D3SIG/DP**3
| E*D3SIG/DP**3 v PT (1) | | (Heavy-flavor decay electrons invariant differential cross-section An additional ... -) |
- - p p --> B... 200 GeV E*D3SIG/DP**3
| E*D3SIG/DP**3 v PT (1) | | (Heavy-flavor decay electrons invariant differential cross-section An additional ... -) |
- - p p --> CHARM... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v Ecm (2) | | (Differential charm cross section To obtain this value, the differential "charm-d... -) |
- - p p --> CHARM... 200 GeV SIG
| SIG v Ecm (3) | | (Total charm cross section To obtain the total charm cross section, the different... -) |
- Adare et al. PRL 103(2009)082002
[R] - 8221472
Measurement of Bottom versus Charm as a Function of Transverse Momentum with Electron-Hadron Correlations in p+p Collisions at sqrt(s)=200 GeV
- - p p --> CHARM... 200 GeV N/N
| N/N v PT (1) | | (Bottom contribution to the electrons from heavy flavor decay as a function of PT... -) |
- - p p --> B... 200 GeV N/N
| N/N v PT (1) | | (Bottom contribution to the electrons from heavy flavor decay as a function of PT... -) |
- - p p --> CHARM... 200 GeV DSIG/DYRAP
- - p p --> B... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v Ecm (2) | | (Differential bottom production cross section at mid rapidity (y=0) To obtain thi... -) |
- - p p --> CHARM... 200 GeV SIG
- - p p --> B... 200 GeV SIG
| SIG v Ecm (6) | | (Total bottom cross section To obtain the total bottom cross section, the differe... -) |
- - p p --> CHARM... 200 GeV E*D3SIG/DP**3
| E*D3SIG/DP**3 v PT (4) | | (Invariant cross section of electrons from charm decay versus PT These values has... -) |
- - p p --> B... 200 GeV E*D3SIG/DP**3
| E*D3SIG/DP**3 v PT (5) | | (Invariant cross section of electrons from bottom decay versus PT These values ha... -) |
- Adare et al. PL B670(2009)313
[R] - 7649452
Dilepton mass spectra in p+p collisions at s**(1/2) = 200-GeV and the contribution from open charm
- - p p --> CHARM... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v Ecm (1) | | (Differential charm cross section at mid rapidity An additional +-39.5 microbarn ... -) |
- - p p --> CHARM... 200 GeV SIG
| SIG v Ecm (2) | | (Total charm cross section An additional systemactic error of +- 200 microbarn, d... -) |
- Adare et al. PR D76(2007)092002
[R] - 6905951
Measurement of Single Muons at Forward Rapidity in p+p Collisions at s**(1/2) = 200-GeV and Implications for Charm Production
- - p p --> CHARM... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v Ecm (1) | | (Differential charm cross section at forward rapidity of 1.6 An additional +0.049... -) |
- 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
- - p p --> J/PSI... 200 GeV SIG
| SIG v Ecm (6) | | (Total cross-section for J/PSI production. The value of the total cross section h... -) |
- - p p --> J/PSI... 200 GeV DSIG/DYRAP
| DSIG/DYRAP v YRAP (5) | | (J/PSI differential cross section times dilepton branching ratio versus rapidity... -) |
- - p p --> J/PSI... 200 GeV D2SIG/DYRAP/DPT
|