重イオン衝突 における 粘性流体描像

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門門 門門 門門門門 () 門門門門門門門門門門門門門 門門 第 19 第 Heavy Ion Café 第第第第 12 第 Heavy Ion Pub 第第第第第 QCD 門門門門門門 2011 門 6 門 8 門 門門門門門

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重イオン衝突 における 粘性流体描像. 門内 晶彦 (東大理). 第 19 回 Heavy Ion Café 並びに第 12 回 Heavy Ion Pub 合同研究会 「 QCD 物質の最前線」、 2011 年 6 月 8 日、名古屋大学. Introduction. “Standard model” of a high-energy heavy ion collision (at RHIC ). t. particles. t. Freezeout . Hadronic cascade. Freezeout. Hydrodynamic stage. - PowerPoint PPT Presentation

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Page 1: 重イオン衝突 における 粘性流体描像

門内 晶彦 (東大理)

重イオン衝突における粘性流体描像

第 19回 Heavy Ion Café並びに第 12回 Heavy Ion Pub合同研究会「 QCD 物質の最前線」、 2011 年 6 月 8 日、名古屋大学

Page 2: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Introduction “Standard model” of a high-energy heavy ion collision (at RHIC)

New Developments

particles

hadronic phase

QGP phase

Freezeout

Pre-equilibrium

Hydrodynamic stage

Color glass condensate

Hadronic cascade

Glasma/Thermalization

Freezeout

z

t

Relativistic hydrodynamicsDescription of collective motion of the QGP (τ ~ 1-10 fm/c)

Discuss the latest experimental data at LHC and RHIC from the perspectives of viscous fluids

Page 3: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

New Developments Higher-order harmonics (v3, v4, v5…)

Higher-Order Harmonics

- Quantified in hydrodynamic models

- Product of initial fluctuations

More observables = more constraints on models

ALICE plenary ATLAS plenary

Page 4: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Higher-Order Harmonics Initial conditions: Glauber (η/s = 1/4π) vs. MC-KLN (η/s = 2/4π)

This does not rule out the KLN

v3 in favor of Glauber?

- η/s would not be indep. of temperature

- Thermalization (CGChydro)

- Bumpy initial conditions may mimic viscosity

PHENIX arXiv:1105.3928

*CGC w/o resonance decay and multiplied by factors obtained in Glauber

Higher-Order Harmonics

Page 5: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Higher-Order Harmonics Shear viscosity: Glauber (η/s = 0) vs. Glauber (η/s = 1/4π)

v3 “has different sensitivity to η/s than v2!”

In other words, no complete data fit by a single η/s (at least for now)  

ALICE (Talk by J. Schukraft)

Higher-Order Harmonics

Bulk viscosity ζ/s ≠ 0 around Tc ; can become non-negligible

CMS (Talk by J. Velkovska)

Page 6: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Higher-Order Harmonics Temperature dependent η/s

Hadronic viscosity always important; QGP viscosity more important at LHC than at RHIC?

Higher-Order Harmonics

Talk by H. Niemi

Poster by C. Shen

Page 7: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Higher-Order Harmonics Flux tubes in initial conditions

Higher-Order Harmonics

vn may depend on “bumpiness” of the initial geometry which mimics viscosity

Talk by Ph. Mota

Page 8: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Higher-Order Harmonics More observables translate into more constraints

Towards Integrated Pictures

- Higher order harmonics in Au-Au and Pb-Pb collisions

- U-U collisions at RHIC for clearer intrinsic v4?- Intrinsic odd-order harmonics (v3, v5…) in asymmetric collisions(e.g. Cu-Pb) ?

Product of fluctuation in initial conditions; centrality independent

Clear centrality dependences may be observed

Possible “other” observables

Page 9: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Towards Integrated Pictures Not only transverse; Longitudinal dynamics

Charged particle multiplicity (0-5%)

CGC

Pb+Pb, 2.76 TeV at η = 0

ALICE: dNch/dη = 1584 ± 4 ± 76CMS: dNch/dη = 1610 ± 55

CGC predictions

dNch/dη ~ 1200?Towards Integrated Pictures

Page 10: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Towards Integrated Pictures CGC rapidity distribution + Full 2nd order viscous hydro

RHIC LHC

Entropy flux

Entropy production

If the true λ is larger at RHIC, it enhances dN/dy at LHC;Hydro effect is an important factor in explaining the LHC data

Currently (1+1)D; (3+1)D viscous hydro under development

AM and T. Hirano, arXiv:1102.5053

Towards Integrated Pictures

Page 11: 重イオン衝突 における 粘性流体描像

Joint Meeting of HIC19 and HIP12 “Frontiers of QCD Matter”, June 8 th 2011, Nagoya

Akihiko Monnai (The University of Tokyo) Viscous Fluids in Heavy Ion Collisions

Next slide:

Towards Integrated Pictures CGC rapidity distribution + Full 2nd order viscous hydro

Currently (1+1)D; (3+1)D viscous hydro under development

RHIC LHC

Entropy flux

Entropy production

If the true λ is larger at RHIC, it enhances dN/dy at LHC;Hydro effect is an important factor in explaining the LHC dataIf the λ is unchanged at RHIC, dN/dy is still enhanced at LHC;Hydro effect is an important factor in explaining the LHC data

AM and T. Hirano, arXiv:1102.5053

Towards Integrated Pictures