Abstract

In this paper we study the behavior of jet quenching parameter in the background metric with hyperscaling violation at finite temperature.The background metric is covariant under a generalized Lifshitz scaling symmetry with the dynamical exponent z and hyperscaling exponent $\theta$. We evaluate the jet quenching parameter for certain range of these parameters consistent with the Gubser bound conditions in terms of T, z and $\theta$. We compare our results with those from conformal case and experimental data. Then we add a constant electric field to this background and find its effect on the jet quenching parameter.

Highlights

  • Holography is a powerful tool to map a D dimensional strongly coupled field theory at large N limit to a D + 1 dimensional gravitational theory at weak coupling [1,2,3,4]

  • We use the gauge/gravity duality to study the behavior of the jet quenching parameter in the background metric with hyperscaling violation at finite temperature with and without a constant B-field

  • The exponent z is the Lifshitz parameter and the exponent θ is the hyperscaling violation exponent, which is responsible for the non-standard scaling of physical quantities and controls the transformation of the metric

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Summary

Introduction

Holography is a powerful tool to map a D dimensional strongly coupled field theory at large N limit to a D + 1 dimensional gravitational theory at weak coupling [1,2,3,4]. We use the gauge/gravity duality to study the behavior of the jet quenching parameter in the background metric with hyperscaling violation at finite temperature with and without a constant B-field. 3, the holographic description of strongly coupled QFT has been applied to illustrate the behavior of the jet quenching parameter at finite temperature. 4, we add a constant B-field (electric field) to the background metric to estimate how the jet quenching parameter depends on the Hawking temperature and the electric field

Review of the background
Jet quenching parameter
Effect of constant electric field
Results and discussion

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