Quarkonia results from PHENIX Raphaël Granier de Cassagnac LLR – École polytechnique Trento, Italia 7 th September 2006.

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Presentation transcript:

Quarkonia results from PHENIX Raphaël Granier de Cassagnac LLR – École polytechnique Trento, Italia 7 th September 2006

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 2 Outline and interests J/ψ in proton-proton –Production mechanisms, reference for dA, AA J/ψ in deuteron-gold –Cold nuclear matter effects, reference for AA From deuteron-gold to nucleus-nucleus –(a personal toy model) J/ψ in nucleus-nucleus –Deconfined quark gluon plasma ? –Still preliminary data from QM05 ! A flash of other quarkonia in proton-proton

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 3 How does PHENIX see the J/ψ ? J/ψ  e + e – identified in RICH and EMCal –|  | < 0.35 –p e > 0.2 GeV/c J/ψ  μ + μ – identified in 2 fwd spectrometers –1.2 < |  | < 2.4 –p μ > 2 GeV/c Centrality and vertex given by BBC in 3<|  |<3.9 and ZDC

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 4 J/ψ in PHENIX YearIons  s NN LuminosityStatusJ/ψ (ee + μμ) 2000Au-Au130 GeV1 μ b -1 Central (electrons) Au-Au200 GeV24 μ b -1 Central [1] 2002 p-p200 GeV0.15 pb muon arm [2] 2002 d-Au200 GeV2.74 nb -1 Central [3] 2003 p-p200 GeV0.35 pb muon arms [3] Au-Au200 GeV241 μ b -1 preliminary~ [4] 2004Au-Au63 GeV9 μ b -1 analysis~ 13 p-p200 GeV350 nb -1 Cu-Cu200 GeV3 nb -1 preliminary~ [4] 2005Cu-Cu63 GeV190 mb -1 analysis~ p-p200 GeV3.8 pb -1 ~ p-p200 GeV10.7 pb -1 Analysis…> [1] PRL92 (2004) PRL92 (2004) [2] PRC69 (2004) PRC69 (2004) [3] PRL96 (2006) PRL96 (2006) [4] QM05, nucl-ex/ nucl-ex/

J/ψ in proton-proton

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 6 Cross section vs rapidity Total cross section  (pp  J/ψ) 2.61 ± 0.20 ± 0.26 μb -Error from fit (incl. syst and stat) -Error on absolute normalization PHENIX, PRL96 (2006)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 7 Cross section versus p T Fit the function = y=1.7 = y=0 [in (GeV/c) 2 ] PHENIX, PRL96 (2006) A (1+(p T /B) 2 ) 6

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 8 p+p perspectives Production mechanism –Color Octet Model does the job In AA (or dA) we have –Large combinatorial background –Low physics backgrounds (Drell-Yan or dileptons from open charm) Run 3 p+p is our baseline –Nuclear modification factor Run 5 & 6 pp analyses going on –Much more statistics, 40 times the luminosity ! R AB = N ψ AB N ψ PP x PRL96, (2006)

J/ψ in deuteron-gold

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 10 d+Au physics motivation Goal: disentangle normal “cold” nuclear effects –Antishadowing & Shadowing (gluon saturation, color glass ?) –Energy loss of initial parton –p T broadening (Cronin effect) –J/ψ (or cc ) absorption –Something else ? Tools: d+Au collisions –over a broad range of p T, rapidity and centrality Interests: –Intrinsically probes interesting nuclear effects –Baseline for Au+Au: Why do J/ψ disappear / appear ? ¯

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 11 Deuteron   Gold In PHENIX, J/  mostly produced by gluon fusion, and thus sensitive to gluon pdf Three rapidity ranges probe different momentum fraction of Au partons –South (y < -1.2) : large x 2 (in gold) ~ –Central (y ~ 0) : intermediate x 2 ~ –North (y > 1.2) : small x 2 (in gold) ~ d Au x1x1 x2x2 J/  in North y > 0 x1x1 x2x2 J/  in South y < 0 rapidity y Eskola, Kolhinen, Vogt NPA696 (2001) 729 An example of gluon shadowing prediction gluons in Pb / gluons in p x Anti Shadowing

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 12 R dA R dAu versus rapidity Data favours –(weak) shadowing Eskola, Kolhinen, Salgado prescription matches better –(weak) absorption σ abs ~ 1 to 3 mb But with limited statistics difficult to disentangle nuclear effects ! PHENIX, PRL96 (2006) Klein,Vogt, PRL91 (2003) Kopeliovich, NPA696 (2001) 669 Low x 2 ~ (shadowing region)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 13 Cross section versus p T Some p T broadening PHENIX, PRL96 (2006)  = dAu – pp Backward: 1.77 ± 0.37 (GeV/c) 2 Mid: [ ± 0.94 (GeV/c) 2 ] Forward: 1.12 ± 0.35 (GeV/c) 2

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 14 R dAu versus p T Low x 2 High x 2 Broadening comparable to lower energy (  s = 39 GeV in E866) R dA

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 15 This is the first J/ψ centrality dependence measurement in dA (or pA) ! Black lines: –EKS98 from 0 to 3 mb Coloured lines: –FGS for 3 mb Slopes consistent with shadowing models low x 2 ! High x 2 ~ 0.09 Low x 2 ~ R dA R dAu versus N coll PHENIX, PRL96 (2006)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 16 d+Au perspectives We have seen small nuclear effects ! –Weak shadowing / antishadowing –Weak absorption (~ 1 to 3 mb) –p T broadening similar to lower energies Difficult to disentangle given statistics –Need more luminosity ! But, no large nuclear effect ! –Good news to see J/ψ modification in Au-Au !

J/ψ in nucleus-nucleus (phenix preliminary)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 18 Quick look to open charm Through semileptonic decays (D  e) PHENIX, PRL94 (2005) N coll scaling ~25% systematic uncertainties (without Silicon vertex detector upgrade) 10 to 20 cc pairs ! (  40 acc. STAR)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 19 R AA versus N coll dAu μμ 200 GeV/c CuCu μμ 200 GeV/c AuAu μμ 200 GeV/c J/ψ  μμ Muon arm 1.2 < |y| < 2.2 AuAu ee 200 GeV/c CuCu ee 200 GeV/c J/ψ  ee Central arm –0.35 < y < 0.35 CuCu μμ 62 GeV/c Hugo Pereira da Costa, for PHENIX, QM05, nucl-ex/ J/ψ suppressed by a factor of ~3 !

Opening parenthesis from dA to AA

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 21 How is it SPS ? Normal nuclear absorption does a splendid job in describing pA, SU, peripheral Pb-Pb… exp(-σ abs ρ° L) with L nuclear thickness & σ abs = 4,18 ± 0,35 mb (or sophisticated Glauber model) No need/care for (anti)shadowing NA50, EPJ C39 (2005) 335 See Carlos & Marzia talks ! J/ψ L

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 22 KKS, PLB637(2006)75 From dA to RHIC What is on the market ? First, the dA data are poor… 1.A model of nuclear absorption + (anti)shadowing (Ramona Vogt, nucl-th/ ) 2.σ diss from fits on dA data  exp -(σ diss (y)+σ diss (-y))n 0 L But shadowing doesn’t go like L… (Karsch, Kharzeev & Satz) 3.My own toy model –(next 3 slides) (These errors must be underestimated)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 23 My own toy model (1/3) Data driven, as much as possible… Phenomenological fit to R dA (b)  Plug this in AuAu Glauber model: R AA (y,b AA ) = Σ collisions [ R dA (-y,b 1 ) x R dA (y,b 2 ) ] Works for absorption & shadowing since: production ~ pdf1 x pdf2 x exp –nσ(L 1 +L 2 ) b1b1 b2b2 b AA Y = -1.7 Y = 0 Y = 1.8 R dA b(fm) RGdC, Hard Probes 2006

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 24 My own toy model (2/3) Bands are statistical and systematic errors from dAu No systematics from the method itself (work in progress) Then, I take the average on AuAu centrality classes to compare to data… N coll | y | ~ 1.7 Cold nuclear matter R AA N coll | y | ~ 0 Cold nuclear matter R AA

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 25 My own toy model (3/3) Comparison to Ramona’s model and AuAu data… Anomalous suppression ≥ 1/3 Uncertainty Normal suppression Vogt, nucl-th/ RGdC, Hard Probes 2006 Error bar code : bars = statistical, bracket = systematic, box : global.

Closing parenthesis Back to (preliminary) AA

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 27 “NA50 only” effects  Capella, Ferreiro, EPJC42 (2005) 419 Grandchamp et al, PRL92 (2004) Kotstyuk et al, PRC68 (2003)  Digal, Fortuno, Satz, EPJC32 (2004) Private communications + (no cold effects) Cold effects + … Comovers (hadrons or partons?) Kinetic model (J/ψ  c c ) Thermal plasma All overestimate suppression ! So does parton percolation  –Onset at N part ~ 90 –Simultaneous J/ψ + χ c + ψ’ (AuAu only)

Is something new affecting RHIC energies ? (I will answer “yes” once and “no” twice)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 29 1 st. Recombination ? A variety of recombination & coalescence models can accommodate the suppression… cc  J/ψ “ But early results suggest some competing mechanism, such as reformation of J/ψ particles, may occur at these densities. ” Riordan & Zajc, Scientific American Amount of regeneration not precisely know (open charm ? phase space ?) To know more, look at y, p T … Grandchamp et al, PRL92 (2004) Bratkoskaya et al, PRC69 (2004) Andronic et al, PLB571 (2003) 36 Thews & Mangano, PRC73 (2006) c + Private communications + See Also David and Anton’s talk yesterday (AuAu only)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 30 y shape (vs recombination) Recombination emphasizes quark y-distribution Quark (open charm) y-distribution unknown No significant change in rapidity in data… Recombined only !  Thews & Mangano, PRC73 (2006) c

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 31 (vs Cronin effect) AB = pp +    p T 2 x L [nuclear matter thickness] (random walk of initial gluons) VN Tram, Moriond 2006 & PhD thesis Lower energy survey pp, pA and AA RHIC (y~1.7)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 32 Cronin versus recombination 1.At forward rapidity (closed symbols) from pp & dA: = L (L N coll conversion) No sign of recombination ! 2.At mid rapidity (open symbols) Negligible Cronin !?... Need better pp ! VN Tram, Moriond 2006 & PhD thesis Bob Thews, Hard Probes 2006 p+p d+Au Au+Au Open symbol: y ~ 0 Full & curves: y ~ 2 = L

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 33 2 nd. Hydro + J/ψ transport One detailed QGP hydro + J/ψ transport (Zhu et al) g + J/ψ  c + c Leakage of higher p T J/ψ First published without cold nuclear effects, but here : + Nuclear absorption (1 or 3 mb) + Cronin effect from dAu ok (as on previous slide) Model should be valid for y=0 –But match y=1.7 –(and central y=0) Predicted R AA for y=0 In nucl-th/ , same authors consider regeneration & multiply by ~2 most central Zhu, Zhuang, Xu, PLB607 (2005) private communication

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 34 3 rd (simple) explanation Datta & al, hep-lat/ Alberico & al, hep-ph/ Wong, hep-ph/  Satz, hep-ph/ We may still be here Amount of anomalous suppression depends on cold nuclear effects amplitude But could be as low as 30 to 40% Compatible to feed-down ratio –100 J/ψ ~ 60 J/ψ + 30 χ c + 10 ψ’ –HERAB says 21±5 χ c & 7.0±0.4 ψ’ Recent lattice T d ψ ~ T c –ε x (T d J/ψ ~ 2T c ) 4 = 2 ε c ε d J/ψ ~ 32 ε c ! Wait for LHC to melt J/ψ ?

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 35 3 rd applied to SPS & RHIC Sequential melting scenario –J/ψ survival only –Excited states melting from ψ’ suppression SPS Be careful when showing this! –NA60 and PHENIX are PRELMINARY… –No systematic uncertainties on PHENIX points –No uncertainties from cold nuclear matter effects However, it does a good job and sequential melting clearly is a possibility !... Karsch, Kharzeev & Satz PLB637(2006)75 ??? J/ψ survival probability − Assuming same formation SPS and RHIC…

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 36 A+A perspectives What’s new at RHIC ? 1 st Recombination ? But no sign of y or p T 2 modifications… J/ψ  (N cc ) 2 (but how much is N cc ?) 2 nd J/ψ transport ? High p T J/ψ escape ? 3 rd Sequential melting ? Only excited states melt ? J/ψ still survive ? These three models assume a QGP ! Lots of ingredients needed to answer… –Cold nuclear effects, open charm,…

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 37 Some steps beyond What do we need to answer ? Final AA analysis –Smaller systematic ? –A bit more data and bins –Better pp reference (Run 5) –Elliptic flow measurement ? (  ) More AA statistics ! –Could be run 7 ? Better knowledge of dA baseline ! –Could be run 8 ? Better open charm measurements –Si VTX upgrade (working on it)  First look at other quarkonia –Going on with run 5 & 6 pp… LHC ! Yan, Zhuang, Xu, nucl-th/

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 38 New quarkonia ahead ! Run 5 pp (3 pb -1 ) Hie Wei, Quark Matter 2005 Υ

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 39 New quarkonia ahead ! Run 6 200GeV p+p Invariant Mass (GeV/c 2 ) ψ’ψ’ Work in progress…

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 40 New quarkonia ahead ! PHENIX Run 5 200GeV p+p PHENIX Run 5 200GeV p+p (eeγ - J/ψ) Mass (GeV/c 2 ) χcχc Work in progress…

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 41 New quarkonia ahead ! All numbers are first rough estimates (including trigger and reconstruction efficiencies) for 12 weeks Au+Au run (∫L eff dt ~ 18 nb -1 ) SignalRHIC Exp.ObtainedRHIC I (>2008) RHIC IILHC/ALICE + J/  → e + e  J/  →     PHENIX~800 ~7000 3,300 29,000 45, ,000 9, ,000  → e+e- →  → e+e- →  STAR PHENIX ,200 1,040 2,600 8,400 B → J/  → e + e  B → J/  →     PHENIX ,700 N/A  c → e + e    c →  +    PHENIX ,600 2,900* 117,000* N/A D→KD→K STAR~0.4×10 6 (S/B~1/600) 30,000** 8000 * Large backgrounds, quality uncertain as yet ** Running at 100 Hz min bias + 1 month (= year), P. Crochet, EPJdirect A1, a (2005) and private comm. © T. Frawley, PANIC’05, RHIC-II Satellite Meeting See Thomas’ talk (next)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac Countries; 62 Institutions; 550 Participants* *as of March 2005

What phenixians cannot say… « Trentatré trentini entrarono a Trento, tutti e trentatré, trotterellando. »

Back up slides

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 45 What’s going RHIC ? Shadowing + nuclear absorption (crucial !) PHENIX, QM05, nucl-ex/ Vogt, nucl-th/ Anomalous suppression ≥ 1/3 Error bar code : bars = statistical, bracket = systematic, box : global. 1.2 < |y| < < y < 0.35 Uncertainty Normal suppression

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 46 Quick comparison to NA50 Same magnitude –30% survival prob. No fundamental reason Differences: –Energy density –Cold / hot nuclear effects balance

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 47 Feed down ratio’s ? From HERA-B (pA √s=41.6 GeV) –7.0 ± 0.4 % from ψ’ –21 ± 5 % from χ c –0.065 ± % from B Faccioli, Hard Probes 2006

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 48 Competing recombination/suppression Grandchamp, Rapp, Brown hep-ph/ Thews, hep-ph/

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 49 Rapidity width Width = 1,90  0,32  2 /ndl = 0,55 Simultaneous fit Separated fits  = 2.61  2,54  2 /dof = 0.21  = 1.85  0,53  2 /dof = 0.41  = 1.82  1,00  2 /dof = 1.39 No noticeable change in rapidity width Width pp = 1,75  0,21 ViNham Tram thesis

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 50 Cronin effect  nuclear density,  elastic gluon-nucleon scattering cross section,  ( ) kick given by each scattering and L average thickness of nuclear matter √ s =17.3 GeV : NA50/60 Pb+Pb, In+In √ s = 19.4 GeV : NA3 p+p, NA38 p+Cu, p+U,O+U, S+U √ s = 27.4 GeV : NA50 p+Be, p+Al, p+Cu, p+W √ s = 29.1 GeV :NA51 p+p, p+d, NA50 p+Al, p+W √ s = 38.8 GeV : E866/789/771 Scattering of initial gluons of nucleon before ccbar formation random walk : AA = pp +  ( ) L AA

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 51 More on J/ψ transport model… Zhu, Zhuang, Xu, PLB607 (2005) D hydro Boltzman-type transport Local equilibrium –(0.8 & 0.6 fm/c) –Normal to anomalous T c = 165 MeV T fo = 60 MeV g+Ψ  cc High p T leakage 40% feeddown No in-medium mod. No

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 52 More on J/ψ transport model… In nucl-th/ , same authors consider regeneration & multiply by ~2 most central

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 53 Run6 p+p

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 54 Dielectron pp and dA

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 55 Centrality analysis Au breaks up in our south beam counter Define 4 centrality classes Relate centrality to through Glauber computation = 8.4 ± 0.7 = 3.2 ± 0.3 = 15.0 ± 1.0 South BBC Charge Central Peripheral Counts d and Au participant nucleons BBC North d Au Spectator nucleons BBC South MB

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 56 Centrality analysis BBC charge versus ZDC energy 5-10% 20-25% 15-20% 0-5% 10-15% Most central % = 351 ± 2.9 = 1065 ± 105 Most peripheral 80 – 92.2% = 6.3 ± 1.2 = 4.9 ± 1.2

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 57 X F = X d - X Au  versus X compared to lower  s Not universal versus X 2 : shadowing is not the whole story. Same versus X F for diff  s. Incident parton energy loss ? (high X d = high X F ) Energy loss expected to be weak at RHIC energy. X 2 (in gold) E866, PRL 84, (2000) 3256 NA3, ZP C20, (1983) 101 PHENIX, PRL96 (2006)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 58 How to get x F scaling ?

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 59 J/ψ transverse momentum (run2) Phenomenological + exponential fits of dimuon and dielectron data give mean p T : = 1.80 ± 0.23 (stat) ± 0.16 (sys) GeV/c Color Singlet Model Color Octet Model (from Nayak et al. hep/ph ) COM contribution is dominant, as for high p T J/ Tevatron

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 60 J/  cross section from run 2 Integrated cross-section : RUN2 234 ± 36 (stat) ± 34 (sys) ± 24(abs) μb RUN3 159 nb ± 8.5 % (fit) ± 12.3% (abs) e+e–e+e– +–+– Results consistent with shapes from various models and PDF. Take the PYTHIA shape to extract our cross-section Error from absolute normalization Consistent (1.3 sigma difference)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 61 Naive picture Less absorption Shadowing Energy loss E866 J/  data (4) Full calculation (+ dE/dx & Chi->J/  (1) quark-shad + FS absorp. (3) anti-shad (2) gluon shadowing (Kopeliovich)

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 62 Tuchin & Kharzeev Hard probes 2004 –hep-ph/ Coherent production of charm (open or closed) –(y<0 production time to low to make computation) –Shadowing from CGC computation… Tuchin

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 63 Tuchin & Kharzeev… + absorption for SPS & fermilab

07 th September 2006 Quarkonia in PHENIX - Raphaël Granier de Cassagnac 64 … gold+gold extrapolation …