2020
DOI: 10.1140/epjc/s10052-020-7951-5
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Magneto-vortical effect in strongly coupled plasma

Abstract: Based on a holographic model incorporating both the chiral anomaly and the gravitational anomaly, we study the effect of magneto-vortical coupling on the transport properties of a strongly coupled plasma. The focus of present work is on the generation of a vector charge density and an axial current, as response to vorticity in a magnetized plasma. The transport coefficients parameterizing the vector charge density and axial current are calculated both analytically (in the weak magnetic field limit) and also nu… Show more

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Cited by 10 publications
(8 citation statements)
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“…We first discuss the case γ = 0. For vanishing magnetic fieldB = 0 we find a linear relation between M 5 /T andμ (at least for the values of the axial chemical potential displayed) of the form M 5 /T = −μ/2 which is in agreement with [116]. However for finite magnetic fields, M 5 /T is no longer directly proportional to µ/T as evident from the inset in the lower left corner.…”
Section: Jhep04(2021)078supporting
confidence: 81%
“…We first discuss the case γ = 0. For vanishing magnetic fieldB = 0 we find a linear relation between M 5 /T andμ (at least for the values of the axial chemical potential displayed) of the form M 5 /T = −μ/2 which is in agreement with [116]. However for finite magnetic fields, M 5 /T is no longer directly proportional to µ/T as evident from the inset in the lower left corner.…”
Section: Jhep04(2021)078supporting
confidence: 81%
“…Recall that the axial chemical potential µ is P-odd and C-even. and was computed in [46,47]. The authors found that…”
Section: Computing the Thermodynamic Susceptibilitiesmentioning
confidence: 99%
“…Recently the combined effect of magnetic field and vorticity has been studied by different groups [11][12][13][14][15][16][17]. In particular, it has been proposed by Hattori and Yin that in the limit of strong magnetic field, where lowest Landau level (LLL) approximation is valid, the effect of vorticity is to shift the energy of the LLL states through spin-orbit coupling [11] ∆ ± = ∓ 1 2 sgn(q f )B • ω, (1.1) where the upper and lower signs correspond to particle and anti-particle of both chiralities and q f is the charge of particle.…”
Section: Introductionmentioning
confidence: 99%
“…Though we study vortical and drift perturbations individually at O(∂), the generation of charge density in vortical solution and generation of heat current in drift solution are connected by Onsager relation[16].…”
mentioning
confidence: 99%