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Transport Coefficients of relativistic matter: A detailed formalism with a gross knowledge of their magnitude

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arxiv 2404.01421 v1 pith:7DN7QMCL submitted 2024-04-01 nucl-th cond-mat.stat-mech

classification nucl-thcond-mat.stat-mech
keywords transportfluidrelativisticrelaxationtimecoefficientsdescriptionmatter
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The present review article has attempted a compact formalism description of transport coefficient calculations for relativistic fluid, which is expected in heavy ion collision experiments. Here, we first address the macroscopic description of relativistic fluid dynamics and then its microscopic description based on the kinetic theory framework. We also address different relaxation time approximation-based models in Boltzmann transport equations, which make a sandwich between Macro and Micro frameworks of relativistic fluid dynamics and finally provide different microscopic expressions of transport coefficients like the fluid's shear viscosity and bulk viscosity. In the numeric part of this review article, we put stress on the two gross components of transport coefficient expressions: relaxation time and thermodynamic phase-space part. Then, we try to tune the relaxation time component to cover earlier theoretical estimations and experimental data-driven estimations for RHIC and LHC matter. By this way of numerical understanding, we provide the final comments on the values of transport coefficients and relaxation time in the context of the (nearly) perfect fluid nature of the RHIC or LHC matter.

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Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. On the Wiedemann-Franz law violation in Graphene and quark-gluon plasma systems

    cond-mat.str-el 2024-12 conditional novelty 4.0 of 10

    A covariant Boltzmann equation with one relaxation time yields L/L0 = (3/pi^2)(h/(k_BT))^2 for both graphene and QGP, so the Wiedemann-Franz law fails as the net carrier density approaches zero.

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