QGP viscosity from RHIC data a hydrodynamic perspective

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QGP viscosity from RHIC data -- a hydrodynamic perspective Huichao Song The Ohio State

QGP viscosity from RHIC data -- a hydrodynamic perspective Huichao Song The Ohio State University Lawrence Berkeley National Lab Joint CATHIE/TECHQM Workshop, BNL, Dec 14 -18, 2009 Supported by DOE Thanks for collaborations and discussions from U. Heinz; Thanks for figures and discussions from K. Dusling, A. El, S. Pratt, Z. Xu, and many others 12/14/2009

What is viscosity Shear viscosity – measures the resistance to flow gradients act against

What is viscosity Shear viscosity – measures the resistance to flow gradients act against the buildup of flow anisotropy Bulk viscosity – measures the resistance to expansion act against the buildup of radial flow Heat conductivity – measures the ability of heat transfer Assume: (RHIC&LHC)

Ideal hydrodynamics S. Bass Conservation laws: ideal hydro: local equilibrium - 4 equations -

Ideal hydrodynamics S. Bass Conservation laws: ideal hydro: local equilibrium - 4 equations - 5 unknowns Input: “EOS” -EOS is one of the important factors that influence the expansion of system harder EOS (with larger ) faster expansion

Viscous hydrodynamics S. Bass Conservation laws: ideal hydro: local equilibrium viscous hydro: near equilibrium

Viscous hydrodynamics S. Bass Conservation laws: ideal hydro: local equilibrium viscous hydro: near equilibrium shear pressure tensor bulk pressure:

Viscous hydrodynamics S. Bass Conservation laws: - Israel-Stewart eqns.

Viscous hydrodynamics S. Bass Conservation laws: - Israel-Stewart eqns.

Viscous hydrodynamics S. Bass Conservation laws: - Israel-Stewart eqns. viscous hydro: near-equilibrium system pre-equilibrium

Viscous hydrodynamics S. Bass Conservation laws: - Israel-Stewart eqns. viscous hydro: near-equilibrium system pre-equilibrium dynamics + viscous hydro + hadron cascade Initial conditions final conditions

Viscous hydrodynamics S. Bass Conservation laws: - Israel-Stewart eqns. Input: “EOS” Bjorken appro. :

Viscous hydrodynamics S. Bass Conservation laws: - Israel-Stewart eqns. Input: “EOS” Bjorken appro. : initial and final conditions reduces (3+1)-d hydro to (2+1)-d hydro

Qualitative effects of & on spectra The same initial & final conditions: ideal hydro

Qualitative effects of & on spectra The same initial & final conditions: ideal hydro viscous hydro-shear only spectra -shear viscosity: flatter spectra -bulk viscosity: steeper spectra viscous hydro-bulk only Song & Heinz, 0909

Qualitative effects of & on spectra The same initial & final conditions: ideal hydro

Qualitative effects of & on spectra The same initial & final conditions: ideal hydro viscous hydro-shear only spectra viscous hydro-bulk only radial flow -shear viscosity: flatter spectra; increases radial flow -bulk viscosity: steeper spectra; decreases radial flow Song & Heinz, 0909

Qualitative effects of & on V 2 Song & Heinz, 0909 Elliptic flow v

Qualitative effects of & on V 2 Song & Heinz, 0909 Elliptic flow v 2 -both shear & bulk viscosity suppress V 2 at low PT

Shear viscosity & elliptic flow V 2 Elliptic flow v 2 20 -25% v

Shear viscosity & elliptic flow V 2 Elliptic flow v 2 20 -25% v 2 suppression -V 2 can be used to extract the QGP shear viscosity -For an acurrate extraction of QGP viscosity, one needs very precise V 2 (experimental data & theoretical results)

Shear viscosity & elliptic flow V 2 Elliptic flow v 2 20 -25% v

Shear viscosity & elliptic flow V 2 Elliptic flow v 2 20 -25% v 2 suppression -V 2 can be used to extract the QGP shear viscosity -For an acurrate extraction of QGP viscosity, one needs very precise V 2 (experimental data & theoretical results)

Shear viscosity & elliptic flow V 2 Elliptic flow v 2 20 -25% v

Shear viscosity & elliptic flow V 2 Elliptic flow v 2 20 -25% v 2 suppression Example: If v 2 is increased by 10%, one need to increase by in order to describe the same exp. data -10% uncertainties in V 2 translate into 50% uncertainties for the extracted value of -V 2 can be used to extract the QGP shear viscosity -For an acurrate extraction of QGP viscosity, one needs very precise V 2 (experimental data & theoretical results)

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial eccentricity (Glauber/CGC ; optical/fluctuations) -treatment of hadronic stage and freeze-out procedure: -Eo. S: EOS Q, EOS L + chemical non-equil. HRG EOS -viscosities & relaxation times: -initialization for

 Effects of initial eccentricity on Glauber Luzum & Romatschke, PRC 2008 -Glauber vs.

Effects of initial eccentricity on Glauber Luzum & Romatschke, PRC 2008 -Glauber vs. CGC: ~20 -30% effect on CGC ~100% uncertainties on -event by event fluctuations: talk by A. Dumitru

 Effects of initial eccentricity on Glauber Luzum & Romatschke, PRC 2008 CGC NOT

Effects of initial eccentricity on Glauber Luzum & Romatschke, PRC 2008 CGC NOT so fast ! -Effects from highly viscous & non-chemical equilibrium hadronic stage, bulk viscosity …

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial eccentricity -treatment of hadronic stage and freeze-out procedure: -chemical composition of HRG -effects of highly viscous HRG -Eo. S: -viscosities & relaxation times: -initialization for shear and bulk pressure

 Effects of chemical composition of HRG on PCE vs. CE (HRG) Partial Chemical

Effects of chemical composition of HRG on PCE vs. CE (HRG) Partial Chemical Equilibrium (PCE) vs. Chemical Equilibrium (CE) Ideal hydro 30% P. Huovinen 07 -PCE Eo. S vs. CE Eo. S (ideal hydro): change v 2 by ~30%

 Effects of chemical composition of HRG on PCE vs. CE (HRG) Glauber Ideal

Effects of chemical composition of HRG on PCE vs. CE (HRG) Glauber Ideal hydro 30% CGC P. Huovinen 07 Luzum &Romatschke 08 -PCE Eo. S vs. CE Eo. S (ideal hydro): change V 2 ~30% -Constraining influence ~100% requires: a proper description of partial chemical equilibrium in HRG

 Effects of highly viscous hadronic stage on Ideal hydro 30 -50% T. Hirano

Effects of highly viscous hadronic stage on Ideal hydro 30 -50% T. Hirano -highly viscous hadronic stage: change V 2 ~30 -50% -need viscous hydro + hadron cascade hybrid approach influence ~100 -150%

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial eccentricity -treatment of hadronic stage and freeze-out procedures: -chemical composition of HRG -viscosity of HRG -Eo. S: (EOSQ vs EOSL) -viscosities & relaxation times: -initialization for shear and bulk pressure

Effects from softness of EOS Song & Heinz PRC 08 SM-EOS Q vs. EOS

Effects from softness of EOS Song & Heinz PRC 08 SM-EOS Q vs. EOS L 40% -- softness of EOS: ~5 -10% effects on V 2 ~25% uncertainties on -- EOS L: Katz 05 lattice data for QGP + CE EOS for HRG talk by P. Houvinen --more realistic EOS for hydro 0903 lattice data for QGP + PCE EOS for HRG 30%

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial eccentricity -treatment of hadronic stage and freeze-out procedures: -chemical composition of HRG -viscosity of HRG -Eo. S: (EOSQ vs EOSL) -viscosities & relaxation times: -initialization for shear and bulk pressure

 shear pressure: relaxation times & initialization Song, Ph. D thesis - is insensitive

shear pressure: relaxation times & initialization Song, Ph. D thesis - is insensitive to initializations of -when extracting and relaxation time : one can neglect the uncertainties from ! (since is short) & initialization of

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial

Extracting from V data 2 Input / parameters for viscous hydro -initial conditions: -initial eccentricity -treatment of hadronic stage and freeze-out procedures: -chemical composition of HRG -viscosity of HRG -Eo. S: (EOSQ vs EOSL) - shear pressure: relaxation times and initialization -effects from bulk viscosity

bulk viscosity and relaxation time Bulk viscosity: HRG Relaxation times: QGP also peaks near

bulk viscosity and relaxation time Bulk viscosity: HRG Relaxation times: QGP also peaks near Tc, this plays an important role for bulk viscous dynamics

bulk viscosity and relaxation time Bulk viscosity: HRG QGP Relaxation times: also peaks near

bulk viscosity and relaxation time Bulk viscosity: HRG QGP Relaxation times: also peaks near Tc, this plays an important role for bulk viscous dynamics Zero initialization: large near Tc prevents from growing to large values suppresses bulk viscous effects

bulk viscosity and relaxation time Bulk viscosity: HRG QGP Relaxation times: also peaks near

bulk viscosity and relaxation time Bulk viscosity: HRG QGP Relaxation times: also peaks near Tc, this plays an important role for bulk viscous dynamics N-S initialization: large near Tc keeps large negative value of in phase transition region viscous hydro breaks down ( ) for larger viscous hydro is only valid with small bulk viscous effects on V 2

Uncertainties from bulk viscosity N-S initialization Zero initialization Song & Heinz, 0909 -with a

Uncertainties from bulk viscosity N-S initialization Zero initialization Song & Heinz, 0909 -with a critical slowing down , effects from bulk viscosity effects are much smaller than from shear viscosity bulk viscosity influences V 2 ~5% (N-S initial. ) uncertainties to ~20% (N-S initial. ) <4% (zero initial. ) <15% (zero initial. )

Extracting from RHIC data --the current status of viscous hydrodynamics (uncertainties in V 2

Extracting from RHIC data --the current status of viscous hydrodynamics (uncertainties in V 2 ) -initial conditions: CGC vs. Glauber ~20 -30% -Eo. S: EOS Q, vs. EOS L ~5 -10% -chemical composition of HRG : (PEC vs. CE) ~30% -viscosity of HRG (or equil. HRG vs. non-equil. HRG) : ~3050% -bulk viscosity: ~5%

Luzum & Romatschke, PRC 2008 Glauber CGC Extracting from RHIC data --the current status

Luzum & Romatschke, PRC 2008 Glauber CGC Extracting from RHIC data --the current status of viscous hydrodynamics (uncertainties in ) -initial conditions: CGC vs. Glauber ~100% -Eo. S: EOS Q, vs. EOS L ~25% -chemical composition of HRG : (PEC vs. CE) ~100% -viscosity of HRG (or equil. HRG vs. non-equil. HRG) : ~100150% viscosity: ~20% -bulk conservative upper limit:

Luzum & Romatschke, PRC 2008 Glauber CGC Extracting from RHIC data --the current status

Luzum & Romatschke, PRC 2008 Glauber CGC Extracting from RHIC data --the current status of viscous hydrodynamics (uncertainties in ) -initial conditions: CGC vs. Glauber ~100%recent progress: Heinz et al. 0907 -Eo. S: EOS Q, vs. EOS L ~25% -chemical composition of HRG : (PEC vs. CE) ~100% -viscosity of HRG (or equil. HRG vs. non-equil. HRG) : ~100150% viscosity: ~20% -bulk conservative upper limit: Can we further increase the accuracy of extracted ? YES !

Luzum & Romatschke, PRC 2008 Glauber CGC Extracting from RHIC data --the current status

Luzum & Romatschke, PRC 2008 Glauber CGC Extracting from RHIC data --the current status of viscous hydrodynamics (uncertainties in ) -initial conditions: CGC vs. Glauber ~100%recent progress: Heinz et al. 0907 -Eo. S: EOS Q, vs. EOS L ~25% -chemical composition of HRG : (PEC vs. CE) ~100% -viscosity of HRG (or equil. HRG vs. non-equil. HRG) : ~100150% viscosity: ~20% -bulk conservative upper limit: -To further decrease the uncertainties from bulk viscosity, (or to extract both shear & bulk viscosity from exp. data), one need more sensitive exp. observables

other observables that are sensitive to - v 2/ε: dependence on system size &

other observables that are sensitive to - v 2/ε: dependence on system size & shear viscosity -photon spectra -HBT radii … …

System size dependence of shear viscous effects Song & Heinz PRC 08 -larger shear

System size dependence of shear viscous effects Song & Heinz PRC 08 -larger shear viscous suppression of elliptic flow in smaller systems

System size dependence of shear viscous effects Song & Heinz PRC 08 -larger shear

System size dependence of shear viscous effects Song & Heinz PRC 08 -larger shear viscous suppression of elliptic flow in smaller systems -the slope of the multiplicity scaling of v 2/ε is sensitive to the value of shear viscosity

System size dependence of shear viscous effects Song & Heinz PRC 08 -larger shear

System size dependence of shear viscous effects Song & Heinz PRC 08 -larger shear viscous suppression of elliptic flow in smaller systems -the slope of the multiplicity scaling of v 2/ε is sensitive to the value of shear viscosity

System size dependence of shear viscous effects Song & Heinz PRC 08 -larger shear

System size dependence of shear viscous effects Song & Heinz PRC 08 -larger shear viscous suppression of elliptic flow in smaller systems -the slope of the multiplicity scaling of v 2/ε is sensitive to the value of shear viscosity

 Multiplicity scaling of v 2/ε Song & Heinz PRC 08 -the slope of

Multiplicity scaling of v 2/ε Song & Heinz PRC 08 -the slope of the multiplicity scaling of v 2/ε is sensitive to the value of shear viscosity -to reproduce the experimental data (slope), a constant is not enough!

 Multiplicity scaling of v 2/ε Song & Heinz PRC 08 -the slope of

Multiplicity scaling of v 2/ε Song & Heinz PRC 08 -the slope of the multiplicity scaling of v 2/ε is sensitive to the value of shear viscosity -to reproduce the experimental data (slope), a constant -data indicate: smaller viscous effects in QGP; is not enough! larger viscous effects in HRG -need viscous hydro + hadron cascade hybrid approach or inputting

other observables that are sensitive to - v 2/ε: dependence on system size &

other observables that are sensitive to - v 2/ε: dependence on system size & shear viscosity -photon spectra -HBT radii … …

EM probes: Photons Photon spectra Pion spectra K. Dusling, 0903 -Viscous hardening of PT-spectra

EM probes: Photons Photon spectra Pion spectra K. Dusling, 0903 -Viscous hardening of PT-spectra is stronger for photons than hadrons -However, earlier thermalization also leads to harder photon spectra (Dusling 0903) -Photon spectra MAY HELP to constrain the 2 -d range of QGP viscosity & thermalization time, together with other observables (V 2 …)

other observables that are sensitive to - v 2/ε: dependence on system size &

other observables that are sensitive to - v 2/ε: dependence on system size & shear viscosity -photon spectra -HBT radii … …

HBT radii S. Pratt QM 09 without viscosity with viscosity - is sensitive to

HBT radii S. Pratt QM 09 without viscosity with viscosity - is sensitive to the QGP viscosity - However, viscosity is only one of the many ingredients that affect HBT radii (Pratt QM 09) - HBT HELPS to constrain the QGP viscosity, together with other observables (V 2 …)

Recent theroetical developments in viscous hydrodynamics - PT-dependent of viscous modification of the particle

Recent theroetical developments in viscous hydrodynamics - PT-dependent of viscous modification of the particle distributions Talk by D. Teaney and D. Molnar - in multi-component systems - 3 rd order viscous hydrodynamics - 3+1 -d viscous hydro: Talk by G. Denicol Talk by A. El Several groups are working on it (MSU, Frankfurt, Krakow, etc)

A short summary - is sensitive to A first attempt to constrain from RHIC

A short summary - is sensitive to A first attempt to constrain from RHIC data indicates BUT: to extract QGP viscosity, one must consider (at least) all the following aspects: - a realistic EOS: - initial conditions: - bulk viscosity: - hadronic stage : EOS L vs. SM-EOS Q, PCE vs. CE CGC vs. Glauber initialization, optical vs. fluctuations uncertainties from bulk viscosity viscous hydro+ hadron cascade …… ……

Thank You

Thank You

EOS

EOS

Qualitative effects of & on V 2 Song & Heinz, 0909 Elliptical flow v

Qualitative effects of & on V 2 Song & Heinz, 0909 Elliptical flow v 2 ideal hydro viscous hydro (shear only) Change the flow profile during hydro evolution Flow + spectra correc. Spectra correc. : viscous hydro (bulk only) (with only flow correction here) A. Monnai talk : spectra correc. for bulk viscosity -v 2 is sensitive to viscosity, especially shear viscosity

EM probes: Photons Photon spectra K. Dusling, 0903 -Photon spectra are more sensitive to

EM probes: Photons Photon spectra K. Dusling, 0903 -Photon spectra are more sensitive to QGP shear viscosity than hadrons -Photon spectra are also sensitive to hydro starting time -Photon spectra may HELP to constrain QGP shear viscosity and hydro starting time -More sophisticated theoretical modeling in the future: including photon emitted from hadronic stage with modified photon emission rate, etc ; better experimental data

S. Pratt QM 09 -To describe the experimental data, one need to consider the

S. Pratt QM 09 -To describe the experimental data, one need to consider the contribution from all kinds of aspects besides shear viscosity

the effects from different initializations -Heinz, Moreland Song

the effects from different initializations -Heinz, Moreland Song

the effects from different initializations -Heinz, Moreland Song

the effects from different initializations -Heinz, Moreland Song

Glauber CGC

Glauber CGC

Glauber CGC

Glauber CGC