effects of bulk viscosity on p t -spectra and elliptic flow parameter
DESCRIPTION
Effects of Bulk Viscosity on p T -Spectra and Elliptic Flow Parameter. Akihiko Monnai Department of Physics, The University of Tokyo, Japan Collaborator: Tetsufumi Hirano. Quark Matter 2009 March 30 th - April 4 th , 2009, Knoxville , TN, U.S.A. arXiv:0903.4436 [nucl-th]. - PowerPoint PPT PresentationTRANSCRIPT
Effects of Bulk Viscosity on pT-Spectra and Elliptic Flow Parameter
Akihiko MonnaiDepartment of Physics, The University of Tokyo, JapanCollaborator: Tetsufumi Hirano
Quark Matter 2009March 30th- April 4th, 2009, Knoxville, TN, U.S.A. arXiv:0903.4436 [nucl-th]
Outline
Outline Introduction - Hydrodynamic models and the Cooper-Frye formula at freezeout
Theories and Methods - Distortion of the distribution from bulk viscosity for a multi-component system in
Grad’s 14-moment method
Numerical Results
- Viscous effects on particle spectra and elliptic flow coefficient v2(pT)
Summary
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Outline Introduction (I)
Outline
Introduction (I)
Paech & Pratt (‘06)Mizutani et al. (‘88) Kharzeev & Tuchin (’08) …
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Success of ideal hydrodynamic models
Development of viscous hydrodynamic models
for the QGP created in relativistic heavy ion collisions
(1) to understand of the hot QCD matter better(2) to constrain the EoS and the transport coefficients from experimental data
Importance of bulk viscositysince it would become large near the QCD phase transition.
In this work, we will see the effects of bulk viscosity at freezeout.
Introduction (I) Introduction (II)Outline
Outline
Introduction (II) Hydrodynamic analyses needs the Cooper-Frye formula at freezeout (i) for comparison with experimental data, (ii) as an interface to a cascade model.
Viscous corrections come in two ways:
(3+1)-D viscous hydro required. We estimate this for a multi-component gas.
Cooper & Frye (‘74)
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Introduction (II)Introduction (I) Relativistic Kinetic Theory
variation of the flow modification of the distribution
* :normal vector to the freezeout hypersurface element, :distribution of the ith particle, :degeneracy.
particles
hadronresonancegas
QGP
freezeout hypersurface Σ
Outline
Relativistic Kinetic Theory Discussion to express in terms of macroscopic variables for a single-component
gas by Israel & Stewart (‘79) The macroscopic variables:
Bulk pressure (1):
Energy current (3):
Charge current (3):
Shear tensor (5):
To ensure thermodynamic stability:
Landau matching conditions (2): ,
where and . : Energy-momentum tensor : Net baryon number current
In Multi-Component SystemIntroduction (II)
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Relativistic Kinetic Theory
Outline
In Multi-Component System Kinetic definitions for a multi-component gas:
where gi is the degeneracy and bi is the baryon number.
We express in terms of macroscopic variables for a multi-component system in Grad’s 14-moment method.
Note: kinetic definitions (12) + matching conditions (2) = 14 equations.
Grad’s 14-moment method
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
In Multi-Component SystemRelativistic Kinetic Theory
Outline
Grad’s 14-moment method Distortion of the distribution expressed with 14 (= 4+10) unknowns:
where + for bosons and – for fermions.
[tensor term ] vs. [scalar term + traceless tensor term ]
Grad’s 14-moment method
The trace part The scalar term
particle species dependent(mass dependent)
particle species independent(macroscopic quantity)
Decomposition of Moments
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
In Multi-Component System
NOT equivalent for a multi-component system.
Outline
Decomposition of Moments Definitions:
*Contributions are : [baryons] + [anti-baryons] + [mesons] : [baryons] – [anti-baryons]
Comments on Quadratic AnsatzGrad’s 14-moment method Decomposition of Moments
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Outline
Comments on Quadratic Ansatz Previous study of the bulk viscosity for a massless gas in QGP with the quadratic
ansatz:
It violates thermodynamic stability (matching conditions) as , .
Note (i) It is not unique; , or ? (ii) Explicit treatment of a multi-component system is necessary.
We will derive without this assumption for a multi-component gas. * remains meaningful in the zero net baryon density limit i.e. .
Comments on Quadratic AnsatzDecomposition of Moments
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Dusling & Teaney (‘08)
Prefactors in Viscous Correction
Outline
Prefactors in Viscous Correction Insert the distribution function into the conditions:
where , , and . The unique form of the deviation is determined:
where, and are functions of ’s and ’s.
Comments on Quadratic Ansatz
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Prefactors in Viscous Correction EoS, Transport Coefficients and Flow
Scalar terms
Vector terms
Tensor term
Outline
EoS, Transport Coefficients and Flow Equation of state:16-component hadron resonance gas *mesons and baryons with mass up to . is taken.
Transport coefficients: ,
where is the sound velocity and s the entropy density.
Freezeout temperature: Tf = 0.16(GeV)
and ( ).
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Weinberg (‘71)Kovtun et al.(‘05)
Hirano et al.(‘06)
…
EoS, Transport Coefficients and FlowPrefactors in Viscous Correction
Profiles of the flow and the freezeout hypersurface : a (3+1)-dimensional ideal hydrodynamic simulation.
pT-Spectra
Outline
pT-Spectra Au+Au, , b = 7.2(fm), pT -spectra of
Model of the bulk pressure:
: free parameter
The bulk viscosity lowers <pT> of the particle spectra.
Elliptic Flow Coefficient v2(pT)pT-Spectra
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
EoS, Transport Coefficients and Flow
Outline
Elliptic Flow Coefficient v2(pT) Au+Au, , b = 7.2(fm), v2(pT) of
The bulk viscosity enhances v2(pT).
*Viscous effects might be overestimated for:
(1) No relaxation for is from the Navier-Stokes limit.
(2) Derivatives of are larger than those of real viscous flow
Results with Quadratic Ansatz
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
pT-Spectra Elliptic Flow Coefficient v2(pT)
Outline
Results with Quadratic Ansatz pT -spectra and v2(pT) of with and the same EoS
Results with Quadratic Ansatz Summary
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Effects of the bulk viscosity is underestimated in quadratic ansatz.
Elliptic Flow Coefficient v2(pT)
Outline
Summary & Outlook Consistent determination of for a multi-particle system A non-zero trace tensor term is needed for the hadron resonance gas up to the
mass of
Visible effects of on particle spectra
Bulk viscosity should be considered to constrain the transport coefficients with better accuracy from experimental data.
A (3+1)-dimensional viscous hydrodynamic flow is necessary to see more realistic behavior of the particle spectra.
SummaryResults with Quadratic Ansatz
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
pT-spectra : suppressed
v2(pT) : enhancedwhen estimated with an ideal hydrodynamic flow.
Outline
Thank You The numerical code for calculations of ’s, ’s and the prefactors shown in
this presentation will become an open source in near future at
http://tkynt2.phys.s.u-tokyo.ac.jp/~monnai/distributions.html
Thank You
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Outline
Summary & Outlook Consistent determination of for a multi-particle system A non-zero trace tensor term is needed for the hadron resonance gas up to the
mass of
Visible effects of on particle spectra
Bulk viscosity should be considered to constrain the transport coefficients with better accuracy from experimental data.
A (3+1)-dimensional viscous hydrodynamic flow is necessary to see more realistic behavior of the particle spectra.
SummaryResults for Shear Viscosity Results for Shear + Bulk ViscosityResults with Quadratic Ansatz
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
pT-spectra : suppressed
v2(pT) : enhancedwhen estimated with an ideal hydrodynamic flow.
Outline
Results for Shear Viscosity pT -spectra and v2(pT) of with , , and the same
EoS.
Results for Shear ViscositySummary Results for Shear + Bulk Viscosity
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Outline
Results for Shear + Bulk Viscosity pT -spectra and v2(pT) of with , , and the same
EoS.
Results for Shear + Bulk ViscosityResults for Shear Viscosity Shear Viscosity in Blast Wave Model
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Outline
Shear Viscosity in Blast Wave Model Effects of the shear viscosity on v2(pT) at freezeout was previously estimated for a
pion gas.
Different when in a single component gas and in a multi-component gas - Shear viscous correction is not so different when and is taken from
the 1st order theory because
in Boltzmann approximation.
Shear Viscosity in Blast Wave Model
Teaney (‘03)
Viscous Flow vs. Viscous DistributionResults for Shear + Bulk Viscosity
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Outline
Viscous Flow vs. Viscous Distribution Corrections via the distortion of distribution function are of the same order as that of
the viscous flow:
Viscous Flow vs. Viscous Distribution
Song & Heinz (‘08)
Shear Viscosity in Blast Wave Model Freezeout Hypersurface
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Outline
Freezeout Hypersurface Comparison of freezeout hypersurfaces for the ideal and the (2+1)-D viscous
hydrodynamics:
Freezeout Hypersurface Expansion of DistributionViscous Flow vs. Viscous Distribution
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Song & Heinz (‘08)
Outline
Expansion of Distribution The distribution function is expanded as follows:
where the momentum expansion is used.
Expansion of Distribution The Matching Conditions
=
Freezeout Hypersurface
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Outline
The Landau matching conditions are necessary to ensure the thermodynamic stability in the 1st order theory:
The Matching Conditions
The Matching ConditionsExpansion of Distribution
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Terms proportional to destabilize the system.
Numerical Results (Prefactors)
Outline
The prefactors for and in ’s near Tf:
Numerical Results (Prefactors)
Numerical Results (Prefactors)
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Trace Part vs. Scalar TermThe Matching Conditions
Outline
Trace Part vs. Scalar Term Separation of the trace part:
works as a free parameter; a single mass dependence can be absorbed.
If we have the scalar term in , , , and diverge at a temperature below Tc.
Trace Part vs. Scalar Term
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Prefactors in Special CaseNumerical Results (Prefactors)
Outline
Prefactors in Special Case We consider : the Landau frame i.e. the zero net baryon density limit i.e. for analyses of heavy ion collisions.
- Apparently vanishes, BUT it does yield a finite relation:
Here, ratios of two ’s remain finite as since
and the chemical potential ’s cancel out.
The number of equations does not change in the process.
Prefactors in Special Case
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Trace Part vs. Scalar Term Explicit Forms of Prefactors
Outline
Explicit Forms of Prefactors The prefactors in the viscous correction tensors are:
where,
Explicit Forms of Prefactors
Quark Matter 2009, Knoxville, Tennessee, April 2nd 2009Effects of Bulk Viscosity on pT-spectra and Elliptic Flow Parameter
Prefactors in Special Case