Abstract

We study the Langevin diffusion of a relativistic heavy quark in anisotropic strongly coupled theories in the local limit. Firstly, we use the axion space-dependent deformed anisotropic N=4 sYM, where the geometry anisotropy is always prolate, while the pressure anisotropy may be prolate or oblate. For motion along the anisotropic direction we find that the effective temperature for the quark can be larger than the heat bath temperature, in contrast to what happens in the isotropic theory. The longitudinal and transverse Langevin diffusion coefficients depend strongly on the anisotropy, the direction of motion and the transverse direction considered. We analyze the anisotropy effects to the coefficients and compare them to each other and to them of the isotropic theory. To examine the dependence of the coefficients on the type of the geometry, we consider another bottom-up anisotropic model. Changing the geometry from prolate to oblate, certain diffusion coefficients interchange their behaviors. In both anisotropic backgrounds we find cases that the transverse diffusion coefficient is larger than the longitudinal, but we find no negative excess noise.

Highlights

  • To examine the dependence of the coefficients on the type of the geometry, we consider another bottom-up anisotropic model

  • For motion along the anisotropic direction we find that the effective temperature for the quark can be larger than the heat bath temperature, in contrast to what happens in the isotropic theory

  • In this paper we have studied the Langevin diffusion coefficients in strongly coupled anisotropic plasmas

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Summary

Generic study of the trailing string and setup

We briefly review some of the generic results of [48] focusing on the ones we need to apply to study the anisotropic theories. The trailing string corresponding to a quark moving on the boundary along the chosen direction xp, p = 1, 2, 3, with a constant velocity has the usual parametrization t = τ, u = σ, xp = v t + ξ(u),. With gαβ being the induced world-sheet metric, we solve for ξ′ in terms of the momentum flowing from the boundary to the bulk, which is a constant of motion ξ′2. The world-sheet of the string has a horizon obtained by gττ (σh) = 0 and turns out to be the same with critical point u0. They are obtained by solving the equation (2.5).

Langevin coefficients
Generalization of the Einstein relation for generic theories
Space-dependent axion deformed background
Bottom-up anisotropic backgrounds
Small anisotropy
Large anisotropy
Langevin diffusion coefficients in bottom-up model
Oblate and prolate geometries
Common results between the two models
Summary and discussion
A Analytic results for small anisotropy
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