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      A study on the collective behavior of chiral plasma using first and second order conformal hydrodynamics

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          Abstract

          We study the collective behaviour of a chiral plasma, for the first and second order conformal hydrodynamics. We have shown that in the early Universe, when the Universe was in thermal equilibrium and there was an asymmetry in the number densities of right and left handed particles, few modes grow exponentially for the values of wave number \(k \leq \xi^B\). However, by using conformal first order hydro, we have shown that in a quasi-equilibrium state of the chiral plasma, waves moving parallel or perpendicular to the background magnetic field, get split into two modes similar to the fast and slow hydrodynamic modes in the standard plasma. However, for the second order conformal hydrodynamics, dispersion relation has a series of terms proportional to different powers of \(k\). These terms are in accordance with the results obtained using ADS/CFT correspondence.

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          Most cited references26

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          Shear viscosity of strongly coupled N=4 supersymmetric Yang-Mills plasma

          , , (2010)
          Using the anti-de Sitter/conformal field theory correspondence, we relate the shear viscosity \eta of the finite-temperature N=4 supersymmetric Yang-Mills theory in the large N, strong-coupling regime with the absorption cross section of low-energy gravitons by a near-extremal black three-brane. We show that in the limit of zero frequency this cross section coincides with the area of the horizon. From this result we find \eta=\pi/8 N^2T^3. We conjecture that for finite 't Hooft coupling (g_YM)^2N the shear viscosity is \eta=f((g_YM)^2N) N^2T^3, where f(x) is a monotonic function that decreases from O(x^{-2}\ln^{-1}(1/x)) at small x to \pi/8 when x\to\infty.
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            Hydrodynamics with Triangle Anomalies

            , (2013)
            We consider the hydrodynamic regime of theories with quantum anomalies for global currents. We show that a hitherto discarded term in the conserve current is not only allowed by symmetries, but is in fact required by triangle anomalies and the second law of thermodynamics. This term leads to a number of new effects, one of which is chiral separation in a rotating fluid at nonzero chemical potential. The new kinetic coefficients can be expressed, in a unique fashion, through the anomalies coefficients and the equation of state. We briefly discuss the relevance of this new hydrodynamic term for physical situations, including heavy ion collisions.
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              New Developments in Relativistic Viscous Hydrodynamics

              Starting with a brief introduction into the basics of relativistic fluid dynamics, I discuss our current knowledge of a relativistic theory of fluid dynamics in the presence of (mostly shear) viscosity. Derivations based on the generalized second law of thermodynamics, kinetic theory, and a complete second-order gradient expansion are reviewed. The resulting fluid dynamic equations are shown to be consistent for all these derivations, when properly accounting for the respective region of applicability, and can be applied to both weakly and strongly coupled systems. In its modern formulation, relativistic viscous hydrodynamics can directly be solved numerically. This has been useful for the problem of ultrarelativistic heavy-ion collisions, and I will review the setup and results of a hydrodynamic description of experimental data for this case.
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                Author and article information

                Journal
                2016-09-07
                Article
                1609.01848
                48067cb4-2184-4b8a-844b-0aab47ff9f53

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                7 pages
                hep-ph astro-ph.CO hep-th physics.plasm-ph

                Plasma physics,Cosmology & Extragalactic astrophysics,High energy & Particle physics

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