Abstract

In this manuscript we explicitly compute the effective dimension of spacetime in some backgrounds of Hořava–Lifshitz (H–L) gravity. For all the cases considered, the results are compatible with a dimensional reduction of the spacetime to d+1=2, at high energies (ultraviolet limit), which is confirmed by other quantum gravity approaches, as well as to d+1=4, at low energies (infrared limit). This is obtained by computing the free energy of massless scalar and gauge fields. We find that the only effect of the background is to change the proportionality constant between the internal energy and temperature. Firstly, we consider both the non-perturbative and perturbative models involving the matter action, without gravitational sources but with manifest time and space symmetry breaking, in order to calculate modifications in the Stephan–Boltzmann law. When gravity is taken into account, we assume a scenario in which there is a spherical source with mass M and radius R in thermal equilibrium with radiation, and consider the static and spherically symmetric solution of the H–L theory found by Kehagias–Sfetsos (K–S), in the weak and strong field approximations. As byproducts, for the weak field regime, we used the current uncertainty of the solar radiance measurements to establish a constraint on the ω free parameter of the K–S solution. We also calculate the corrections, due to gravity, to the recently predicted attractive force that black bodies exert on nearby neutral atoms and molecules.

Highlights

  • The Horava-Lifshitz (H-L) gravity is an alternative proposal to quantum gravity theory, recently presented in the literature, which is power-counting renormalizable [1,2,3]

  • In this paper we have analyzed implications on the black body radiation which is derived from the dynamics of massless scalar and gauge fields in two different situations, with and without a gravitational source in the framework of the Horava-Lifshitz theory

  • For the case with source we have supposed that the black body has mass M and radius R generating a static, spherically symmetric and asymptotically flat background gravity described by the Kehagias-Sfetsos solution

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Summary

INTRODUCTION

The Horava-Lifshitz (H-L) gravity is an alternative proposal to quantum gravity theory, recently presented in the literature, which is power-counting renormalizable [1,2,3]. The connection between the phenomenology involving gravity and thermodynamics was studied in the early seventies of past century [27, 28], and reexamined more recently [29, 30] In this context, Black Holes seem to be the objects of the universe in which these connections become stronger, and any modifications in the laws derived from thermodynamics due to gravitational effects must consider these structures, necessarily. Black Holes seem to be the objects of the universe in which these connections become stronger, and any modifications in the laws derived from thermodynamics due to gravitational effects must consider these structures, necessarily In this scenario, black body radiation is emblematic, in view of the possible role played by this phenomenon in the construction of a quantum theory of gravity.

Non-perturbative Model
Perturbative Model
BLACK BODY RADIATION DUE TO A SPHERICAL GRAVITATIONAL SOURCE
Weak-field approximations
Strong-field approximations
THE “BLACK BODY FORCE”
Findings
CONCLUDING REMARKS
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