Data for Rapidity_Distributions

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... -)

• 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 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 v YRAP (3)

    (J/PSI distribution in rapidity. The data at rapidity = 0 is from the electron ar... -)

• 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 v YRAP (1)

    (J/PSI differential cross section in P+P reactions( times di-lepton branching rat... -)

  • - d A --> J/PSI... 200 GeV

    DSIG/DYRAP v YRAP (2)

    (J/PSI nuclear modification factor RDA,as a function of rapidity.... 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 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... -)

• 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 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... -)

  • - p p --> J/PSI... 200 GeV

    DSIG/DYRAP v YRAP (5)

    (J/PSI differential cross section times dilepton branching ratio versus rapidity... -)

• 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 :... -)

• 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
  
  • - d A --> J/PSI... 200 GeV

    D2N/DPT/DYRAP v CENTRALITY (8)

    (J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus centrality at forward rapid... Au)

    D2N/DPT/DYRAP v CENTRALITY (7)

    (J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus centrality at mid rapidity ... Au)

    D2N/DPT/DYRAP v CENTRALITY (6)

    (J/PSI invariant (1/(2PI*PT))*D2(N)/DPT/DYRAP versus centrality at backward rapi... Au)

    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)

• 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

    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

    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... -)

• 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 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 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

    DSIG/DYRAP v Ecm (2)

    (Differential charm cross section To obtain this value, the differential "charm-d... -)

• 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
  • - p p --> B... 200 GeV

    DSIG/DYRAP v Ecm (2)

    (Differential bottom production cross section at mid rapidity (y=0) To obtain thi... -)

• 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 v Ecm (1)

    (Differential charm cross section at mid rapidity An additional +-39.5 microbarn ... -)

• 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 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

    DSIG/DYRAP v YRAP (5)

    (J/PSI differential cross section times dilepton branching ratio versus rapidity... -)

• 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
  
  • - p p --> J/PSI... 200 GeV

    D2SIG/DPT/DYRAP v PT (1)

    (J/psi differential production cross section 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
• Abelev et al. PRL 94(2005)062301 [R] - 5922518
  Open charm yields in d + Au collisions at s(NN)**(1/2) = 200-GeV
  
  • - d A --> CHARM... 200 GeV

    DSIG/DYRAP v Ecm (6)

    (D0 differential yield at mid rapidity and corresponding calculated differential ... Au)

    DSIG/DYRAP v Ecm (7)

    (Sum of the non photonic electrons/positrons and D0 differential yield at mid rap... Au)

• 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

    DSIG/DYRAP v PLAB (4)

    (Differential cross section at rapidity zero for P NUCLEON --> J/PSI X.... NUCLEON,C,Ti,Wt)

• 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

    YRAP 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

    YRAP v MEAN(XL) (2)

    (Target Atomic Mass dependence expressed as the POWER for PSIPRIME production. X2... Be,Fe,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
  
  • - p A --> J/PSI... 800 GeV

    DSIG/DYRAP v YRAP (4)

    (Location: T 4... Nucleon,Au)

  • - p A --> PSI... 800 GeV

• Abe et al. PRL 75(1995)4358 [R] - 3196933
  Upsilon production in p anti-p collisions at s**(1/2) = 1.8-TeV
  
  • - pbar p --> UPSI... 1800 GeV

    DSIG/DYRAP v PT (1)

    (SIG*Br(UPSI --> MU+ MU-)... -)

    DSIG/DYRAP v PT (2)

    (SIG*Br(UPSI --> MU+ MU-)... -)

  • - pbar p --> UPSI... 1800 GeV

    D2SIG/DPT/DYRAP v PT (5)

    (The first (asymmetric) systematic error represents the uncertainty in the decay ... -)

    D2SIG/DPT/DYRAP v PT (6)

    (The first (asymmetric) systematic error represents the uncertainty in the decay ... -)

    D2SIG/DPT/DYRAP v PT (7)

    (The first (asymmetric) systematic error represents the uncertainty in the decay ... -)

• Acosta et al. PRL 88(2002)161802 [R] - 4840046
  Upsilon production and polarization in p anti-p collisions at s**(1/2) = 1.8-TeV
  
  • - pbar p --> UPSI... 1800 GeV

    D2SIG/DPT/DY v PT (1)

    (The differential cross section times the branching ratio into mu+ mu- for UPSILO... -)

    D2SIG/DPT/DY v PT (2)

    (The differential cross section times the branching ratio into mu+ mu- for UPSILO... -)

    D2SIG/DPT/DY v PT (3)

    (The differential cross section times the branching ratio into mu+ mu- for UPSILO... -)

• Acosta et al. PR D66(2002)092001 [R] - 5406900
  Cross-section for forward J / psi production in p anti-p collisions at S = 1.8-TeV
  
  • - pbar p --> J/PSI... 1800 GeV

    DSIG/DETARAP v ETARAP (1)

    (The integrated cross section for J/PSI --> MU+ MU- decay.... -)

  • - pbar p --> J/PSI... 1800 GeV

    D2SIG/DETARAP/DPT v PT (2)

    (Cross section as a function of PT. Statistical errors only.... -)

• Aaltonen et al. PRL 102(2009)242001 [R] - 8164398
  Observation of exclusive charmonium production and gamma gamma ---> mu+mu- in p anti-p collisions at s**(1/2) = 1.96-TeV
  
  • - pbar p --> P PSI... 1960 GeV

    DSIG/DYRAP v YRAP (2)

    (Prompt Psi(2S) cross section from exclusive photoproduction at mid rapidity... -)

  • - pbar p --> P CHI... 1960 GeV

    DSIG/DYRAP v YRAP (4)

    (chi_c0 cross section from exclusive double pomeron production at mid rapidity... -)

• Abbott et al. PRL 82(1999)35 [R] - 3805468
  Small angle J / psi production in p anti-p collisions at S**(1/2) = 1.8-TeV
  
  • - pbar p --> J/PSI... 1800 GeV

    D2SIG/DETARAP/DPT v PT (1)

    (Only statistical errors are shown. Cross section tines branching ratio... -)

• Abbott et al. PRL 84(2000)5478 [R] - 4129156
  Small angle muon and bottom quark production in p anti-p collisions at S**(1/2) = 1.8-TeV
  
  • - pbar p --> B... 1800 GeV

    D2SIG/DPT/DYRAP v PT (2)

    (The cross section for muons originating from b-quark decay... -)

  • - pbar p --> MU... 1800 GeV

    D2SIG/DPT/DYRAP v PT (1)

    (The forward muon cross section (per unit rapidity)... -)

    D2SIG/DPT/DYRAP v PT (2)

    (The cross section for muons originating from b-quark decay... -)

• Abazov et al. PRL 94(2007)232001 [R] - 6133959
  Measurement of inclusive differential cross sections for Upsilon(1S) production in p anti-p collisions at s**(1/2) = 1.96-TeV
  
  • - pbar p --> UPSI... 1960 GeV

    DSIG/DYRAP v YRAP (1)

    (Cross section per unit of rapidity times branching ratio to MU+ MU-. Systematic ... -)

  • - pbar p --> UPSI... 1960 GeV

    D2SIG/DPT/DYRAP v PT (2)

    (Normalized differential cross section for UPSI(1S) production.. Errors contain s... -)

• Badier et al. PL 86B(1979)98 [R] - 393754
  FIRST EVIDENCE FOR UPSILON PRODUCTION BY PIONS
  
  • - pi+ A --> UPSI... 200 GeV

    DSIG/DYRAP v YRAP (1)

    (Location: 1... Nucleus,Pt)

  • - pi- A --> UPSI... 200,280 GeV

    DSIG/DYRAP v YRAP (1)

    (Location: 1... Nucleus,Pt)

    DSIG/DYRAP v YRAP (2)

    (Location: 2... Nucleus,Pt)

• Barlag et al. PL 302B(1993)112 [R] - 2877643
  Charmed pair correlations in pi- Cu interactions at 230-GeV/c.
  
  • - pi- A --> D... 230 GeV

    YRAP,M,PT v P (1)

    (FOR ONLY 20 EVENTS IN WICH BOTH DECAYS ARE FULLY RECONSTRUCTED ( 26 D0 , 8 D+ , ... Cu,Nucleus)

    YRAP,M,PT v P (2)

    (Location: T2... Cu,Nucleus)

• Barlag et al. CERN-EP-88-104 [R] - 1893386
  RESULTS ON LAMBDA(c)+, D(s)+, D0 AND D+ PRODUCTION PROPERTIES IN 230-GeV/c pi- Cu INTERACTIONS FROM THE NA32 EXPERIMENT
  
  • - pi- A --> CHARM... 230 GeV

    M,XL,PT,YRAP v P (17)

    (Location: T 4... Cu,Nucleus)

• Albajar et al. PL B200(1988)380 [R] - 1759256
  HIGH TRANSVERSE MOMENTUM J / psi PRODUCTION AT THE CERN PROTON - ANTI-PROTON COLLIDER
  
  • - pbar p --> J/PSI... 630 GeV

    DSIG/DYRAP v YN (3)

    (Data extracted from figure with g3data... -)

• Albajar et al. PL B209(1988)397 [R] - 1822233
  LOW MASS DIMUON PRODUCTION AT THE CERN PROTON - ANTI-PROTON COLLIDER
  
  • - pbar p --> MU... 630 GeV

    ED3SIG/DP3 v PT (1)

    (GLOBAL SYTEMATIC ERROR OF 30PCT HAS TO BE ADDED... -)

• Aamodt et al. CERN-PH-EP-2011-057 [R] - 9050507
  Rapidity and transverse momentum dependence of inclusive J/psi production in pp collisions at sqrt(s) = 7 TeV
  
  • - p p --> J/PSI... 7000 GeV

    D2SIG/DPT/DYRAP v PT (2)

    (Differential J/PSI cross section from the di-muon channel as a function of trans... -)

    D2SIG/DPT/DYRAP v PT (1)

    (Double differential J/PSI cross section from the di-electron channel as a functi... -)

  • - p p --> J/PSI... 7000 GeV

    DSIG/DYRAP v YRAP (3)

    (Differential J/PSI cross section from the di-electron and di-muon channel as a f... -)

• Aamodt et al. JHEP 1201(2011)128 [R] - 9258736
  Measurement of charm production at central rapidity in proton-proton collisions at $\\sqrt{s} = 7$ TeV
  
  • - p p --> D... 7000 GeV

    DSIG/DYRAP v RE (4)

    (Integrated cross sections for prompt charm particle production extraplated to PT... -)

• Aamodt et al. PL B708(2012)265 - 9340173
  Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV
  
  • - p p --> MU... 7000 GeV
• 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-2012-021 - 9375368
  $J/\psi$ Production as a Function of Charged Particle Multiplicity in $pp$ Collisions at $\sqrt{s} = 7$ TeV
  
  • - p p --> J/PSI... 7000 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

• Aad et al. CERN-PH-EP-2011-041 [R] - 9035664
  Measurement of the differential cross-sections of inclusive, prompt and non-prompt J/psi production in proton-proton collisions at sqrt(s) = 7 TeV
  
  • - p p --> J/PSI... 7000 GeV

    D2SIG/DPT/DYRAP v PT (22)

    (Summary table of all sources of considered systematic uncertainty and statistica... -)

    D2SIG/DPT/DYRAP v PT (21)

    (Summary table of all sources of considered systematic uncertainty and statistica... -)

    D2SIG/DPT/DYRAP v PT (20)

    (Summary table of all sources of considered systematic uncertainty and statistica... -)

    D2SIG/DPT/DYRAP v PT (18)

    (Prompt J/psi production cross-sections as a function of J/psi pT for J/psi rapid... -)

    D2SIG/DPT/DYRAP v PT (17)

    (Prompt J/psi production cross-sections as a function of J/psi pT for J/psi rapid... -)

    D2SIG/DPT/DYRAP v PT (16)

    (Prompt J/psi production cross-sections as a function of J/psi pT for J/psi rapid... -)

    D2SIG/DPT/DYRAP v PT (15)

    (Prompt J/psi production cross-sections as a function of J/psi pT for J/psi rapid... -)

    D2SIG/DPT/DYRAP v PT (14)

    (Non-prompt J/psi production cross-sections as a function of J/psi pT for J/psi r... -)

    D2SIG/DPT/DYRAP v PT (13)

    (Non-prompt J/psi production cross-sections as a function of J/psi pT for J/psi r... -)

    D2SIG/DPT/DYRAP v PT (12)

    (Non-prompt J/psi production cross-sections as a function of J/psi pT for J/psi r... -)

    D2SIG/DPT/DYRAP v PT (11)

    (Non-prompt J/psi production cross-sections as a function of J/psi pT for J/psi r... -)

    D2SIG/DPT/DYRAP v PT (6)

    (Inclusive J/psi production cross-section as a function of J/psi pT in the J/psi ... -)

    D2SIG/DPT/DYRAP v PT (5)

    (Inclusive J/psi production cross-section as a function of J/psi pT in the J/psi ... -)

    D2SIG/DPT/DYRAP v PT (4)

    (Inclusive J/psi production cross-section as a function of J/psi pT in the J/psi ... -)

    D2SIG/DPT/DYRAP v PT (3)

    (Inclusive J/psi production cross-section as a function of J/psi pT in the J/psi ... -)

    D2SIG/DPT/DYRAP v PT (23)

    (Summary table of all sources of considered systematic uncertainty and statistica... -)

  • - p p --> B... 7000 GeV

    D2SIG/DPT/DYRAP v PT (18)

    (Prompt J/psi production cross-sections as a function of J/psi pT for J/psi rapid... -)

    D2SIG/DPT/DYRAP v PT (17)

    (Prompt J/psi production cross-sections as a function of J/psi pT for J/psi rapid... -)

    D2SIG/DPT/DYRAP v PT (16)

    (Prompt J/psi production cross-sections as a function of J/psi pT for J/psi rapid... -)

    D2SIG/DPT/DYRAP v PT (15)

    (Prompt J/psi production cross-sections as a function of J/psi pT for J/psi rapid... -)

    D2SIG/DPT/DYRAP v PT (14)

    (Non-prompt J/psi production cross-sections as a function of J/psi pT for J/psi r... -)

    D2SIG/DPT/DYRAP v PT (13)

    (Non-prompt J/psi production cross-sections as a function of J/psi pT for J/psi r... -)

    D2SIG/DPT/DYRAP v PT (12)

    (Non-prompt J/psi production cross-sections as a function of J/psi pT for J/psi r... -)

    D2SIG/DPT/DYRAP v PT (11)

    (Non-prompt J/psi production cross-sections as a function of J/psi pT for J/psi r... -)

• Aad et al. PL B705(2011)9 - 9111808
  Measurement of the Upsilon(1S) Production Cross-Section in pp Collisions at sqrt(s) = 7 TeV in ATLAS
  
  • - p p --> UPSI... 7000 GeV

• Aaij et al. CERN-PH-EP-2011-018 [R] - 8987840
  Measurement of J/psi production in pp collisions at sqrt(s)=7 TeV
  
  • - p p --> J/PSI... 7000 GeV

    DSIG/DYRAP v YRAP (5)

    (DSIG/DY for prompt (unpolarised) J/PSI and from b-hadron decay integrated over P... -)

  • - p p --> B... 7000 GeV

    DSIG/DYRAP v YRAP (5)

    (DSIG/DY for prompt (unpolarised) J/PSI and from b-hadron decay integrated over P... -)

  • - p p --> J/PSI... 7000 GeV

    D2SIG/DPT/DYRAP v PT (7)

    (Double differential cross section in PT and YRAP for J/PSI from b-hadron decays ... -)

    D2SIG/DPT/DYRAP v PT (6)

    (Double differential cross section in PT and YRAP for prompt J/PSI production ass... -)

    D2SIG/DPT/DYRAP v PT (8)

    (Double differential cross section in PT and YRAP for prompt J/PSI production ass... -)

    D2SIG/DPT/DYRAP v PT (9)

    (Double differential cross section in PT and YRAP for prompt J/PSI production ass... -)

  • - p p --> B... 7000 GeV

    D2SIG/DPT/DYRAP v PT (7)

    (Double differential cross section in PT and YRAP for J/PSI from b-hadron decays ... -)

• Aaij et al. CERN-PH-EP-2012-051 - 9393412
  Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV
  
  • - p p --> UPSI... 7000 GeV

• Khachatran et al. CERN-PH-EP-2010-046 [R] - 8875847
  Prompt and non-prompt J/psi production in pp collisions at sqrt(s) = 7 TeV
  
  • - p p --> J/PSI... 7000 GeV

    D2N/DPT/DYRAP v PT (4)

    (Differential inclusive cross J/PSI section for the |rapidity| range 1.6 to 2.4 f... -)

    D2N/DPT/DYRAP v PT (3)

    (Differential inclusive cross J/PSI section for the |rapidity| range 1.2 to 1.6 f... -)

    D2N/DPT/DYRAP v PT (2)

    (Differential inclusive cross J/PSI section for the |rapidity| range 0 to 1.2 for... -)

    D2N/DPT/DYRAP v PT (8)

    (Differential prompt J/PSI cross section for the |rapidity| range 0 to 1.2 for ea... -)

    D2N/DPT/DYRAP v PT (9)

    (Differential prompt J/PSI cross section for the |rapidity| range 1.2 to 1.6 for ... -)

    D2N/DPT/DYRAP v PT (10)

    (Differential prompt J/PSI cross section for the |rapidity| range 1.6 to 2.4 for ... -)

    D2N/DPT/DYRAP v PT (11)

    (Differential non-prompt J/PSI cross section for the |rapidity| range 0 to 1.2.... -)

    D2N/DPT/DYRAP v PT (12)

    (Differential non-prompt J/PSI cross section for the |rapidity| range 1.2 to 1.6.... -)

    D2N/DPT/DYRAP v PT (13)

    (Differential non-prompt J/PSI cross section for the |rapidity| range 1.6 to 2.4.... -)

  • - p p --> B... 7000 GeV

    D2N/DPT/DYRAP v PT (11)

    (Differential non-prompt J/PSI cross section for the |rapidity| range 0 to 1.2.... -)

    D2N/DPT/DYRAP v PT (12)

    (Differential non-prompt J/PSI cross section for the |rapidity| range 1.2 to 1.6.... -)

    D2N/DPT/DYRAP v PT (13)

    (Differential non-prompt J/PSI cross section for the |rapidity| range 1.6 to 2.4.... -)

• Chatrchyan et al. PRL 106(2011)112001 [R] - 8924996
  Measurement of the $B^+$ Production Cross Section in pp Collisions at $\\sqrt{s} = 7$~TeV
  
  • - p p --> B... 7000 GeV

    DSIG/DYRAP v YRAP (3)

    (Measured differential cross section as a function of the rapidity of the B+ part... -)

• Chatrchyan et al. JHEP 1103(2011)090 [R] - 8941262
  Inclusive b-hadron production cross section with muons in pp collisions at sqrt(s) = 7 TeV
  
  • - p p --> B... 7000 GeV

    DSIG/DETARAP v ETARAP (3)

    (Muon pseudorapidity differential distibution.... -)

• Chatrchyan et al. PRL 106(2011)252001 [R] - 9035010
  Measurement of the B0 production cross section in pp Collisions at sqrt(s) = 7 TeV
  
  • - p p --> B... 7000 GeV

    DSIG/DYRAP v YRAP (3)

    (Measured differential cross section as a function of the rapidity of the B0 part... -)

• Chatrchyan et al. PR D84(2011)052008 [R] - 9105441
  Measurement of the Strange B Meson Production Cross Section with J/Psi phi Decays in pp Collisions at sqrt(s) = 7 TeV
  
  • - p p --> B... 7000 GeV

    DSIG/DYRAP v YRAP (3)

    (The measured differential cross section as a function of the rapidity of the B/... -)

• Chatrchyan et al. JHEP 1202(2012)011 [R] - 9258752
  J/psi and psi(2S) production in pp collisions at sqrt(s) = 7 TeV
  
  • - p p --> J/PSI... 7000 GeV

    D2SIG/DPT/DYRAP v PT (1)

    (The (unpolarised) acceptance corrected J/PSI cross section times branching ratio... -)

    D2SIG/DPT/DYRAP v PT (2)

    (The (unpolarised) acceptance corrected J/PSI cross section times branching ratio... -)

    D2SIG/DPT/DYRAP v PT (3)

    (The (unpolarised) acceptance corrected J/PSI cross section times branching ratio... -)

    D2SIG/DPT/DYRAP v PT (4)

    (The (unpolarised) acceptance corrected J/PSI cross section times branching ratio... -)

    D2SIG/DPT/DYRAP v PT (5)

    (The (unpolarised) acceptance corrected J/PSI cross section times branching ratio... -)

    D2SIG/DPT/DYRAP v PT (9)

    (The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for... -)

    D2SIG/DPT/DYRAP v PT (10)

    (The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for... -)

    D2SIG/DPT/DYRAP v PT (11)

    (The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for... -)

    D2SIG/DPT/DYRAP v PT (12)

    (The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for... -)

    D2SIG/DPT/DYRAP v PT (13)

    (The uncorrected visible J/PSI cross section times branching ratio to MU+ MU- for... -)

    D2SIG/DPT/DYRAP v PT (29)

    (The difference between the J/PSI cross section times branching ratio to MU+ MU- ... -)

    D2SIG/DPT/DYRAP v PT (30)

    (The difference between the J/PSI cross section times branching ratio to MU+ MU- ... -)

    D2SIG/DPT/DYRAP v PT (31)

    (The difference between the J/PSI cross section times branching ratio to MU+ MU- ... -)

    D2SIG/DPT/DYRAP v PT (32)

    (The difference between the J/PSI cross section times branching ratio to MU+ MU- ... -)

    D2SIG/DPT/DYRAP v PT (33)

    (The difference between the J/PSI cross section times branching ratio to MU+ MU- ... -)

  • - p p --> PSI... 7000 GeV

    D2SIG/DPT/DYRAP v PT (6)

    (The (unpolarised) acceptance corrected PSI(2S) cross section times branching rat... -)

    D2SIG/DPT/DYRAP v PT (7)

    (The (unpolarised) acceptance corrected PSI(2S) cross section times branching rat... -)

    D2SIG/DPT/DYRAP v PT (8)

    (The (unpolarised) acceptance corrected PSI(2S) cross section times branching rat... -)

    D2SIG/DPT/DYRAP v PT (14)

    (The uncorrected visible PSI(2S) cross section times branching ratio to MU+ MU- f... -)

    D2SIG/DPT/DYRAP v PT (15)

    (The uncorrected visible PSI(2S) cross section times branching ratio to MU+ MU- f... -)

    D2SIG/DPT/DYRAP v PT (16)

    (The uncorrected visible PSI(2S) cross section times branching ratio to MU+ MU- f... -)

    D2SIG/DPT/DYRAP v PT (34)

    (The difference between the PSI(2S) cross section times branching ratio to MU+ MU... -)

    D2SIG/DPT/DYRAP v PT (35)

    (The difference between the PSI(2S) cross section times branching ratio to MU+ MU... -)

    D2SIG/DPT/DYRAP v PT (36)

    (The difference between the PSI(2S) cross section times branching ratio to MU+ MU... -)

• Chatrchyan et al. CERN-PH-EP-2012-036 [R] - 9383875
  Inclusive b-jet production in pp collisions at sqrt(s)=7 TeV
  
  • - p p --> B... 7000 GeV

    DSIG/DPT/DYRAP v PT (4)

    (Inclusive b-jet double-differential cross sections and their ratio to inclusive ... -)

    DSIG/DPT/DYRAP v PT (5)

    (Inclusive b-jet double-differential cross sections and their ratio to inclusive ... -)

    DSIG/DPT/DYRAP v PT (6)

    (Inclusive b-jet double-differential cross sections and their ratio to inclusive ... -)

    DSIG/DPT/DYRAP v PT (7)

    (Inclusive b-jet double-differential cross sections and their ratio to inclusive ... -)

    DSIG/DPT/DYRAP v PT (8)

    (Inclusive b-jet double-differential cross sections and their ratio to inclusive ... -)

  • - p p --> B... 7000 GeV

    DSIG/DYRAP v YRAP (11)

    (Inclusive b-jet (with muon) differential cross sections in the PT range greater ... -)

    DSIG/DYRAP v YRAP (12)

    (Inclusive b-jet differential cross sections in the PT range greater than 30 GeV,... -)