Time Evolution and Thermal Renormalization Group Flow in Cosmology

Fuente: arXiv
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Autori principali: Marian, Istvan Gabor, Trombettoni, Andrea, Nandori, Istvan
Natura: Preprint
Pubblicazione: 2024
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author Marian, Istvan Gabor
Trombettoni, Andrea
Nandori, Istvan
author_facet Marian, Istvan Gabor
Trombettoni, Andrea
Nandori, Istvan
contents Time-evolution of the Universe as described by the Friedmann equation can be coupled to equations of motion of matter fields. Quantum effects may be incorporated to improve these classical equations of motion by the renormalization group (RG) running of their couplings. Since temporal and thermal evolutions are linked to each other, astrophysical and cosmological treatments based on zero-temperature RG methods require the extension to finite-temperatures. We propose and explore a modification of the usual finite-temperature RG approach by relating the temperature parameter to the running RG scale as $T \equiv k_T = τk$ (in natural units), where $k_T$ is acting as a running cutoff for thermal fluctuations and the momentum $k$ can be used for the quantum fluctuations. In this approach, the temperature of the expanding Universe is related to the dimensionless quantity $τ$ (and not to $k_T$). We show that by this choice dimensionless RG flow equations have no explicit $k$-dependence, as it is convenient. We also discuss how this modified thermal RG is used to handle high-energy divergences of the RG running of the cosmological constant and to "solve the triviality"of the $ϕ^4$ model by a thermal phase transition in terms of $τ$ in $d=4$ Euclidean dimensions.
format Preprint
id arxiv_https___arxiv_org_abs_2405_07846
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Time Evolution and Thermal Renormalization Group Flow in Cosmology
Marian, Istvan Gabor
Trombettoni, Andrea
Nandori, Istvan
High Energy Physics - Theory
General Relativity and Quantum Cosmology
Time-evolution of the Universe as described by the Friedmann equation can be coupled to equations of motion of matter fields. Quantum effects may be incorporated to improve these classical equations of motion by the renormalization group (RG) running of their couplings. Since temporal and thermal evolutions are linked to each other, astrophysical and cosmological treatments based on zero-temperature RG methods require the extension to finite-temperatures. We propose and explore a modification of the usual finite-temperature RG approach by relating the temperature parameter to the running RG scale as $T \equiv k_T = τk$ (in natural units), where $k_T$ is acting as a running cutoff for thermal fluctuations and the momentum $k$ can be used for the quantum fluctuations. In this approach, the temperature of the expanding Universe is related to the dimensionless quantity $τ$ (and not to $k_T$). We show that by this choice dimensionless RG flow equations have no explicit $k$-dependence, as it is convenient. We also discuss how this modified thermal RG is used to handle high-energy divergences of the RG running of the cosmological constant and to "solve the triviality"of the $ϕ^4$ model by a thermal phase transition in terms of $τ$ in $d=4$ Euclidean dimensions.
title Time Evolution and Thermal Renormalization Group Flow in Cosmology
topic High Energy Physics - Theory
General Relativity and Quantum Cosmology
url https://arxiv.org/abs/2405.07846