Heavy Flavor Measurements at RHIC&LHC W. Xie (Purdue University, West Lafayette) W. Xie (Purdue University, West Lafayette) Open Heavy Flavor Workshop.

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Presentation transcript:

Heavy Flavor Measurements at RHIC&LHC W. Xie (Purdue University, West Lafayette) W. Xie (Purdue University, West Lafayette) Open Heavy Flavor Workshop June 18,

Motivation  Involve different interaction mechanisms from light quarks with the medium  gluon bremsstrahlung radiation  collisional energy loss  collision dissociation  Ads/CFT  Sensitive to initial gluon density and gluon distribution at RHIC.  produced mostly from gluon fusion  Cold Nuclear effect. Gluon shadowing, Color glass condensate, Initial state Energy loss, etc  Reference to Quarkonia production Similar initial state effect. Large cross section (compared to J/ψ).  Accurate reference. D0D0 K+K+  l K-K- e-/-e-/- e-/-e-/- e+/+e+/+ Heavy quarkonia Open heavy flavor NPE 2

RHIC Measurements on NPE R AA large suppression of heavy quark production is observed STAR: PRL 106, (E) (2011) PHENIX: PRL 98, (2007). 3

The Large Suppression of Non-photonic Electron Production was a Surprise D0D0 radiative energy loss c quark K+K+ l e-/-e-/- (Baier et al, Kharzeev et al, Djordjevic et al, Wiedemann et al. ) u c “dead cone effect”: gluon radiation suppressed at  < m Q /E Q collision energy loss c quark Hot/Dense Medium (Teaney et al, Rapp et al, Molnar et al, Gossiaux et al.) D0D0 K+K+ l e-/-e-/- D0D0 meson energy loss c quark u c Hot/Dense Medium Vitev, et al u c D0D0 K+K+ l e-/-e-/- (Gubser et al., Herzog et al., Horowiz, Gyulassy et al.) 4

Do We Understand the Result at RHIC ? We need more differential predictions and measurements DGLV: Djordjevic, PLB632, 81 (2006) BDMPS: Armesto, et al.,PLB637, 362 (2006) T-Matrix: Van Hees et al., PRL100,192301(2008). Coll. Dissoc. R. Sharma et al., PRC 80, (2009). Ads/CFT: W. Horowitz Ph.D thesis. 5

(Some) Predictions at RHIC and LHC DGLV and AdS/CFT W. Horowitz, Ph.D thesis. For both, the magnitude of R AA for charm and bottom are very different. R AA vs. pT shape from the two models are very different. LHC 6

(Some) Predictions at RHIC and LHC 7

Towards Disentangling Charm and Bottom Production at RHIC  ~30-60% of non-photonic electron come from B meson in 200GeV p+p collisions. STAR: Phys. Rev. Lett. 105, (2010) PHENIX: Phys. Rev. Lett. 103, (2009) 8

Separate Measurement of B  e and D  e Spectra at RHIC p+p 200 GeV result ideal to get similar result from Au+Au but it’s a lot harder. STAR Phys. Rev. D 83, (2011) PHENIX Phys. Rev. Lett. 103, (2009) 9

 Combining data from Run2010 &  Total: ~800 M Min.Bias events  Significant signals are observed  In collisions of all centralities The Power of High Luminosity: D 0 Signal in Au+Au 200 GeV 10

D 0 R AA in Au+Au 200 GeV He,Fries,Rapp: PRC86,014903; arXiv: ; private comm.  Suppression at high p T in central and mid-central collisions  Enhancement at intermediate p T.  Radial flow via coalescences with light quarks?  Cronin effect?  Charm and light hadron have similar suppression pattern at high pT. 11

D Meson Production in Pb+Pb 2.76 TeV Run2010 Run2011  Similar level of suppression as RHIC for 2 < pT <6 GeV/c  Clear pathlength dependence  follow light hadron suppression pattern  Similar at RHIC. 12

(J/psi) B suppression in Pb+Pb 2.76 TeV From non-prompt J/psi measurements. Significant B suppression observed. Even at most peripheral bin shadowing? Suppression seems larger at forward rapidity region. 13

B-jet suppression in Pb+Pb 2.76 TeV 14

pT (B meson: GeV/c) counts PYTHIA6 default setting B suppression in Au+Au 200 GeV  Based on NPE R AA at pT > 5 GeV/c and B fraction measurement.  B significantly suppressed  Agree with CMS observation via B->J/psi  Based on NPE and D0 measurements  Indicate suppression of B  Large uncertainty. 15

ALICE Observation of Bottom Suppression. 16

1 probe + 1(other) probe > 2 (separate) probes  Comparison in similar pT region of B and D mesons  Charm suppress more than Bottom  Discrimination power against models. 17

Large CNM Effect Observed at RHIC  Large enhancement in d+Au collision at mid and backward rapidity.  small suppression at low pT at forward rapidity. PHENIX HF e 18

 R pPb (NPE) systematically above 1.0,  same effect as observed by PHENIX ??  But R pPb (D) ~1.0.  Coincidence due to systematics or B  e?  Consistent with the shadowing and CGC.  (Much) larger Cronin effect at RHIC? CNM Effects Observed at LHC 19

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21 What are Expected at Lower Energy

 Note: J/psi not subtracted.  Observe “enhancement” at 62.4 GeV.  Shape = pQCD  Radial flow + CNM enhancement dominate suppression at lower energy? NPE Enhancement also Observed at Lower Energy 22

A (Qualitative) Summary More Differential Measurements & Precision: Luminosity and/or New Tools 23

The New Tools. MTD (MRPC) 24

The Probing Tools 25

Backup slide 26

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