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High p T  0 Production in p+p, Au+Au, and d+Au Stefan Bathe UC Riverside for the Collaboration Topics in Heavy Ion Collisions McGill University, Montreal,

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Presentation on theme: "High p T  0 Production in p+p, Au+Au, and d+Au Stefan Bathe UC Riverside for the Collaboration Topics in Heavy Ion Collisions McGill University, Montreal,"— Presentation transcript:

1 High p T  0 Production in p+p, Au+Au, and d+Au Stefan Bathe UC Riverside for the Collaboration Topics in Heavy Ion Collisions McGill University, Montreal, Canada, June 25-28, 2003

2 HIC03Stefan Bathe2 High p T Particle Production High p T particles in p+p and A+A –result from parton-parton scattering with high Q 2 p+p –fragmentation of partons to hadrons in QCD vacuum A+A –hard scatterings in early stage –high p T partons probe hot and dense nuclear matter formed in later stages Colored quark matter –partons lose energy via gluon bremsstrahlung –jet quenching –suppression of high p T hadrons q q q q

3 HIC03Stefan Bathe3    Charged hadrons –Drift Chamber (DC) –Pad Chamber (PC) PHENIX Setup  0 via  0  –EMCal Lead Scintillator (PbSc) Lead Glass (PbGl) PHENIX Central Arms |  |< 0.35 Event characterization, vertex –Beam Beam Counter (BBC) –3.0 < |  | < 3.9 –Zero Degree Calorimeter (ZDC)

4 HIC03Stefan Bathe4 p+p Collision at = 200 GeV

5 HIC03Stefan Bathe5 Constrains Fragmentation Function D(Gluon-  ) Reference for Au+Au spectra  0 Production in p+p hep-ex/0304038  AB  hX  f a/A (x a,Q 2 a )  f b/B (x b,Q 2 b )  a b  cd  D h/c (z c,Q 2 c ) Good agreement with NLO pQCD –Factorization theorem:

6 HIC03Stefan Bathe6 Au+Au Collision at = 200 GeV

7 HIC03Stefan Bathe7 Centrality Selection in Au+Au Participants charged particles: BBC (3.0 < |  < 3.9) spectator neutrons: ZDC (~18 m from vertex) Spectators Centrality characterized by –N part : Number of nucleons which suffered  1 collision –N coll : Number of inelastic nucleon- nucleon collisions N part and N coll from Glauber calculations

8 HIC03Stefan Bathe8  0 Production in Au+Au Particle Physics central Nuclear Physics peripheral PHENIX Collab. submitted to PRL nucl-ex/0304022 central spectra up to 10 GeV/c NN-reference needed

9 HIC03Stefan Bathe9 Nuclear Modification Factor R AA Hard processes –yield scales with N coll –reason: small cross section incoherent superposition Nuclear Modification Factor R AA In the absence of nuclear effects: R AA =1 at high p T no effect strong suppression

10 HIC03Stefan Bathe10 R AA for  0 in Central Collisions Cronin Effect at lower energies Expectation –R AA > 1 Observed –factor 4-5 suppresion at 130 and 200 GeV A.L.S.Angelis PLB 185, 213 (1987) WA98, EPJ C 23, 225 (2002) PHENIX, PRL 88 022301 (2002) PHENIX submitted to PRL, nucl-ex/0304022

11 HIC03Stefan Bathe11 Jet Quenching?  0 suppression described by models with parton energy loss Additional nuclear effects needed to describe p T dependence Other explanations not ruled out at this stage q q q q without parton energy loss with parton energy loss Wang Levai Vitev Comparison with model calculations with and without parton energy loss:

12 HIC03Stefan Bathe12 Initial Final State Effects Initial state effects –lead to R AA  1 at high p T –but are not related to properties of hot and dense nuclear matter Possibilities –Initial state multiple soft scatterings (Cronin effect) R AA > 1 –Modifications of nuclear structure functions in nuclei (Shadowing) R AA < 1 –gluon saturation (Color Glass Condensate) R AA < 1 ? Final state effects –dense partonic medium parton energy loss (and recombination) –dense hadronic medium hadronic energy loss

13 HIC03Stefan Bathe13 d+Au: The Control Experiment A+A collision N+A collision Initial state nuclear effects present in both A+A and N+A collisions Final state medium effects only present in A+A collisions

14 HIC03Stefan Bathe14 No suppression in d+Au d+Au R AA in d+Au (R dA ) Final state effects minimal in d+Au Initial state effects ruled out as explanation for suppression in Au+Au Au+Au d+Au

15 HIC03Stefan Bathe15  0 in d+Au: Data Theory Data well reproduced by –NLO pQCD calculation, plus –phenomenological model of Cronin effect, plus –Shadowing Levai et al., nucl-th/0306019 Kopeliovich et al., hep-ph/0201010 Cronin Effect: Multiple Collisions broaden high P T spectrum

16 HIC03Stefan Bathe16 Summary Strong suppression of high p T particle production in central Au+Au at = 200 GeV with respect to N coll scaled p+p reference No suppression in 200 GeV d+Au Suppression in Au+Au is caused by properties of created hot and dense medium

17 HIC03Stefan Bathe17

18 HIC03Stefan Bathe18 Backup Slides

19 HIC03Stefan Bathe19 Centrality Dependence of Suppression Peripheral (60-92%) consistent with N coll scaling R AA <1 (2  ) for 50- 60% –N part ~ 50  15 –  Bjorken ~ 1.2 GeV/fm 3 Gradual or abrupt suppression not conclusive at this point  Bjorken (GeV/fm 3 ) D.d'Enterria PHENIX Collab. nucl-ex/0306001

20 HIC03Stefan Bathe20 d+Au Spectra Final spectra for charged hadrons and identified pions. Data span 7 orders of magnitude.

21 HIC03Stefan Bathe21 R AA vs. R dA for Identified  0 d+Au Au+Au Initial State Effects Only Initial + Final State Effects

22 HIC03Stefan Bathe22 Systematic Errors (1  ) Peak extraction geometric acc.  0 reconstr. Eff. Energy scale Trigger eff. G1 Norm. Scale Conv. Correction Total error p T indep. 5.0%(5.0%) 2.8%(2.8%) 2 GeV 3.0%(3.0%) 4.0%(4.0%) - 10%(10%) 6 GeV 2.0%(2.0%) 4.0%(4.0%) 9.0%(9.0%) 5.0%(10.0%) 14%(16%) 10 GeV 2.0%(2.0%) 4.5%(4.5%) 11.0%(11.0%) 3.0%(3.0%) 15%(15%) type A B C PbSc (PbGl)

23 HIC03Stefan Bathe23 Charged Hadron Results d+Au Au+Au

24 HIC03Stefan Bathe24 First grasp at centrality selection in dAu IR 18 m ZDC FCAL p n ZDC Neutron tagged events are enhanced in very-peripheral collisions

25 HIC03Stefan Bathe25 First grasp at centrality selection in dAu IR ZDC FCAL p n ZDC FCAL Energy Deposit

26 HIC03Stefan Bathe26 R dA / R pA Comparison of very-peripheral events ( =3.6+/-0.4) to minimum bias events ( =8.5+/-0.7) Data indicates no centrality dependence

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