High-p T Particles and RHIC Paradigm of Jet Quenching Ahmed M. Hamed NN2012 The 11 th International Conference on Nucleus-Nucleus Collisions 1.

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Presentation transcript:

High-p T Particles and RHIC Paradigm of Jet Quenching Ahmed M. Hamed NN2012 The 11 th International Conference on Nucleus-Nucleus Collisions 1

2 RHIC and QCD Phase Diagram  Condensed Matter (SSB) → Cosmology, Finite Temperature Field Theory  QCD matter (T ≈ 100 MeV) → Relativistic Heavy Ion Collisions ( QGP ) ? o Bag Model based model o Nambu-Jona-Lasinio- NJL model o Statistical Thermal model o Chiral Perturbation Theory o Lattice QCD Theory of QCD phase diagram

3  fragmentation of partons scattered with large momentum transfer High-pt Particles early time of the collisions (0.1 fm/c) rates in the framework of pQCD Jet high-pt, leading, particle high momentum transfer (exchange) p p Yield = fractional energy carried by initial parton*hard scattering (parton interactions)*fractional energy carried by final particles

STAR, nucl-ex/ energy loss Deduced ε ≈ 15 GeV/fm 3 ~ 15*ε critical (e.g. X.N. Wang nucl-th/ ) SYSTEM NEEDS TO BE PARTONIC 4 Yield (AA) Yield (pp) R AA = RHIC Paradigm of Jet Quenching-I  ≠ 1 → not incoherent superposition of pp collisions.  ≈ 0.2 → large suppression beyond CNM effect.

5 RHIC Paradigm of Jet Quenching-II Surface emissions picture Au+Au Surface bias ? PRL 91 (2003) Recoil jet → quenched inside the medium Jet quenching is final state effect

6 Hadrons (light quarks) → not calibrated probes RHIC Paradigm of Jet Quenching-III pQCD-based models → wide rang of medium parameters.

7 Calibrated Probes P(  E)  f ( E, L, C R, m)‏ 1) E: parton initial energy 2) L: path length 3) C R : color factor (q/g) 4) m: quark mass  hh h Surface bias → Direct photon → Direct photon/hadrons → hadrons (Q)/hadrons (q) 2), and 3) → recoil jet from h to lose more energy than that of  dir → Light quarks (q) are expected to lose more energy than heavy quarks (Q)

Phys. Rev. C 82, (2010) 8 The yields in p+p and Au+Au are well described by theory Recoil jet of direct photon-I = vs. Phys. Rev. C 82, (2010) I AA D AA D NN = Energy loss is independent of parton initial (negligible k T !)

9 o Conditional yield per π 0 and direct photon triggers show similar level and pattern of suppression over wide range of centrality as R AA of π 0 and charged hadrons (light and heavy) Recoil jet of direct photon-II Centrality dependence

10 Phys. Rev. C 82, (2010) Recoil jet of direct photon-III Unexpected similar level and pattern of suppression, challenge to theory! Fragmentation photons? Dominance of fluctuations in energy loss? Lower z T ? Different techniques (STAR/PHENIX) → similar results

11 Conclusions  QCD phase diagram is of very rich structure and exploring these phases is a key theme of modern nuclear physics  The only mean (so far) to study hot nuclear matter is RHIC  High-p T particles are crucial signature for QGP  Single hadron and di-jet analysis at mid  in pp, dAu, and AuAu support the final state effect “jet quenching” in AA  Theory - experiment comparison support the partonic energy loss (light quarks) over the hadronic absorptions  Associated yields with direct photons show similar medium effect as those associated with hadrons!  Calibrated probe/particle’s Id measurements have been started at RHIC; many detector upgrades; and collider machine as well, stay tuned. Spanish poet Antonio Machado: (Traveller, the road is nothing more than your footprints; Traveller, there is no road, you make it as you go.