2017
DOI: 10.1007/jhep05(2017)001
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Relativistic magnetohydrodynamics

Abstract: Abstract:We present the equations of relativistic hydrodynamics coupled to dynamical electromagnetic fields, including the effects of polarization, electric fields, and the derivative expansion. We enumerate the transport coefficients at leading order in derivatives, including electrical conductivities, viscosities, and thermodynamic coefficients. We find the constraints on transport coefficients due to the positivity of entropy production, and derive the corresponding Kubo formulas. For the neutral state in a… Show more

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Cited by 144 publications
(356 citation statements)
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“…8 The Kubo formulas (3.23) and (3.27)-(3.29) agree with those presented in Ref. [36]. We thank Pavel Kovtun for discussions regarding these matters.…”
Section: B Kubo Formulassupporting
confidence: 81%
See 1 more Smart Citation
“…8 The Kubo formulas (3.23) and (3.27)-(3.29) agree with those presented in Ref. [36]. We thank Pavel Kovtun for discussions regarding these matters.…”
Section: B Kubo Formulassupporting
confidence: 81%
“…This inaccuracy was pointed out to us by the authors of Ref. [36], and we thank them for bringing this to our attention. expansion (3.11) and (3.12) into (3.16) and neglecting the fluid gradient terms, we find that the electric field created by this current source is…”
Section: ð3:8þmentioning
confidence: 74%
“…In [7] (see also earlier work in [8,9]) the hydrodynamic theory of such a system at finite temperature was developed and shown to be equivalent to a generalized form of relativistic magnetohydrodynamics. See also [10] for a recent discussion of magnetohydrodynamics in the conventional formulation.…”
Section: Electromagetism Coupled To Electrically Charged Mattermentioning
confidence: 99%
“…sources; strictly speaking, electromagnetism is a gauge theory and dynamical gauge fields complicate the hydrodynamic description [22,27], although the physics is only qualitatively different under extreme magnetic fields.…”
Section: Jhep06(2017)054mentioning
confidence: 99%
“…In the presence of a finite magnetic field, the viscosity becomes a fourth-rank tensor with multiple non-vanishing coefficients: see e.g. [22,27]. Other contributions are proportional to third-order corrections (in spatial gradients) to the charge current J µ ; these can be thought of as k 2 corrections to the coefficient c in (4.8).…”
Section: Jhep06(2017)054mentioning
confidence: 99%