perspectives on rhic-ii: heavy ions and hot+dense matter

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Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter Ralf Rapp Texas A&M University 1. RHIC-II Science Workshop BNL, 19.11.04

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Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter. Ralf Rapp Texas A&M University 1. RHIC-II Science Workshop BNL, 19.11.04. Introduction I: Hot and Dense QCD. + Thermal Field Theory. 2GeVT energy loss. - PowerPoint PPT Presentation

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Page 1: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

Perspectives on RHIC-II:Heavy Ions and Hot+Dense Matter

Ralf RappTexas A&M University

1. RHIC-II Science WorkshopBNL, 19.11.04

Page 2: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

Introduction I: Hot and Dense QCD2

41

aq Gq)m̂Agi(q QCDL + Thermal Field Theory

pQCD: p>>T energy loss

non-pert QCD: p~T equation of state

2GeV<p<6GeV hadronization

medium probe (1) cluster (2-3) medium response (1000)≈20GeVfm-3 quark scaling thermal, 0≈0.5fm/cD≈0.7GeV

nonabelian?! Mass/binding? phase transition?

RAA(pt)v2(pt/n) / n v2(pt,m)

Page 3: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

Thermalization at RHIC study: • chiral symmetry restoration• deconfinement• spectral properties of matter

Introduction II: Exploring the Phase Diagram

1.0 T/Tc

m‹qq›-

T=1.4Tc

Genuine properties of QGP!Direct link to lattice QCD!

[Bielefeld] L

L

[Tokyo]

Page 4: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

2.) Early Phases Matter Composition and Temperature 3.) QGP at p››T Nonabelian Effects Energy Deposition

4.) QGP at p~T Degrees of Freedom and Interactions Deconfinement

5.) Chiral Symmetry Restoration Order Parameters and Observables Medium Modifications of Hadrons

6.) Other Puzzles and Opportunities 7.) Concluding Remarks

Outline

Page 5: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

2.) Early Matter Composition[Hirano+Nara ‘04]

Initial State: CGC!? (fwd y)

• QGP (=47cT4) or GP (=16cT4)• qq production (CGC, sphalerons)• thermalization at 0≤ 0.5fm/c• initial temperature

Electromagnetic Diagnostics: • photons and dileptons gq→q ~ g q

qq→ee ~ (q )2

• thermal window: q0 , Mee≈ 1-3GeV• pre-equilibrium contribution?!

Page 6: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

3.1 Energy Loss

Eg/Eq=9/4 +increasing gluon content with √s

3.) Probing the QGP with high pt

RA

A(p

t=6G

eV)

√s [GeV]

• L2-DependenceAlready observed in DIS on nuclei [HERMES]

RHIC: medium expansion + centrality dependence L2

• Non-Abelian Charge

• Heavy Quarks mQ provides extra scale to disentangle, e.g., screening mass D

• Energy Gauge: high-pt photon tag; RAA(pt→∞)→1 ?!

[Wang ’04]

[Kharzeev+Dolshitzer, Djordjevic etal]]

[Vitev ’04]

Page 7: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

Cone angle of shock frontcosemis = cs/c em=±(55º-63º)emis

[STAR]pT=(0.15-4)GeV

3.2 Energy Deposition and Correlations

Track “lost” energy: • thermalization?• correlations as advanced tests of coalescence [Hwa etal, Fries etal]• sonic shock wave in the hydrodynamic medium: [Shuryak]

Page 8: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

4.) The Thermal Nature of QGP4.1 Light-Quark SectorHydrodynamics requires early equilibration. How?

Potential scenarios: (i) pQCD + ?! (ii) sQGP: heavy q, g + (many) boundstates (iii) q, g + (few) resonances

large imaginary parts required (liquid: M~ vs. plasma: <<T)

(i) Perturbative QCD Rescattering• “anomalously” large width ~g2T• gg↔ggg rescattering [Xu+Greiner ’04]• nonabelian plasma instabilites [Moore etal ’04]

Page 9: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

(ii) Heavy Partons + Multiple Bound States→ based on finite-T lattice potentials approach to “zero-binding line” ~ stable-mass-resonance

[Shuryak,Zahed, Brown, …]

• thermal parton scattering through bound states?• composite interactions? quark scaling?

Dilepton Radiationratio to pert. qq rate

Mee/mq

_

Page 10: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

(iii) “Hadronic” Resonances (few, colorless) • “moderately” heavy q+g, rescattering above threshold; • “hadron” formation above Tc → generalize coalescence • check with open heavy flavor

• dynamical origin of resonances? cc production? • onset of pQCD regime: pt>5-6GeV ? open bottom?

_ [Müller etal ’95, Molnar’04]

[van Hees+RR ’04]

Thermalization + “D”-Mesons

pQCD

“D”

Ellitpic Flow + Coalescence

jet- quench[Djordjevic etal ’04]

Page 11: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

4.2 Quarkonia: Direct vs. Regeneration QCD Lattice: J/ up to ~2Tc in QGP J/ + g c + c + X←→ -

]NN[d

dN eq

)T/)mmexp[()m/m()N(N c

/ccc

eq 2232

: inelastic reaction rate (width)

• c-quark equilibration?• Deconfinement order parameter? Width?!

[Grandchamp etal]

Centrality Dependence

[Thews]

Rapidity Spectra

mc *

y

J/ Excitation Function

Page 12: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

(ii) Scrutinizing Charmonium Regeneration J/ Elliptic Flow

Furthermore: Bottomonium suppression?! ’ (sensitive to in-medium D-mesons)

Suppression only Thermal Coalescence at Tc

[Wang+Yuan ’02][Greco etal ’04]

MB Au-Au

Factor ~5 different! Transition in pt!?

Page 13: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

5.) Chiral Symmetry Restoration

~ “- a1(1260)” (chiral partners)

Axial-/Vector in Vacuum

pQCD cont.

)Im(Ims

dsf AV

2

Order parameters: <qq> , f, mq* ↔ Relation to observable?

)T(fMqxdd

dN Bee23

2

44

Imem ~ [ImD+ImD/10+ImD/5]

Low-Mass Dilepton Rate:-mesondominated!

at Tc: Chiral

Restoration

-

Page 14: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

Hadronic Many-Body Theory

5.2 Vector Mesons at RHIC

• baryon effects important even at B,net=0 : sensitive to B,tot=+B , most pronounced at low M • more robust ↔ OZI

-

Dilepton Emission Rates

Quark-Hadron Duality ?!in-med HG ≈ in-med QGP !

[qq→ee][qq+O(s)]

--

Page 15: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

5.3 Dileptons I: Lessons from SPS

New Data (preliminary)

• enhancement concentrated at low (pair-) pt , theory low? • signal increases with ~ (Nch )2 • mass region between and

8% centralpt

e >100MeV

Page 16: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

5.3 Dileptons II: RHIC

• low mass: thermal! (mostly in-medium )• connection to Chiral Restoration: a1 (1260)→ , 3• int. mass: QGP vs. cc → e+e-X, softening due to rescatt.? (v┴!)-

[RR ’01]

[R. Averbeck, PHENIX]

QGP

Page 17: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

5.4 Resonance Spectroscopy

Dilute matter, but versatile:• -meson: m=-50MeV and/or broad. + thermal PS + BE ?• →

: threshold strength? (↔)• baryons! ++→+p, N(1535)→N,… • reliable freezeout treatment (transport)

[STAR]

[Florkowski etal, Brown+Shuryak]

Theoretical Opportunities: • ↔ 0++-glueball mixing, connects ‹qq› ↔ ‹L› • interacting hadronic EoS: (B,T) - chem. freezeout - order parameter:

D

C

Temperature T →

Qua

rk M

ass m

q

QCD

mG→0

m→0

[Fukushima]

h hq

h

q mΩ

mm

qq

Page 18: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

6.) (Some) Other Puzzles and Opportunities

• constituent quark scaling accidental? [Molnar]

• HBT: early QGP push + pos. x-t correlation? [Lin+Ko ‘02]

• exotic particles: + [Nonaka etal ’04] ,Bc [Thews ‘99] , glueballs ?

• global QGP polarization at finite b? [Wang ’04]

• P, CP violation (UA(1) restoration)? [Kharzeev ’04]

Page 19: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

7.) Summary• RHIC-II unique (dedicated) facility to unravel genuine (nonpert.) QCD properties of the QGP: - nonabelian energy loss (high-pt) - bound states / resonances (IM-dileptons, open charm) - deconfinement (quarkonia; width?! J/ -regen, -supp) - chiral symmetry restoration (LM-dileptons, resonances) mostly rare probes (incl. excitation functions)• importance of precision data + theory (redundancy) to disentangle mechanisms

very exciting opportunities ahead …

Page 20: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

4.2 Direct Photons and Dileptons

),(1023

2

4 TqfMqd

dR Bee

),( 0230 Tqfqd

dRq B

Sources:• Initial hard scatt.: Drell-Yan / Compton (tag jets! [Gale])• Pre-equilibrium: Radiation off jets [Gale] , rescatt.+fragment. of secondaries (parton cascade [Bass])• Thermal:

Im Πem(M,q)

Im Πem(q0=q)

e+

e-

γe.m. correlator

chemical off-equilibrium: QGP: q,g ≤ 1 HG: ,K,.. > 0

[Niemi,Moore]

Page 21: Perspectives on RHIC-II: Heavy Ions and Hot+Dense Matter

Direct Photons at SPS and RHIC

• large “pre-equilibrium” yield from parton cascade (no LPM)• thermal yields ~ consistent• QGP undersaturation small effect

• pQCD Cronin ~ π0

T0≈205MeV sufficient• new WA98 points: -Bremsstr. via soft ?

[Turbide etal]