Barrow Cosmology and Big-Bang Nucleosynthesis

Fuente: arXiv
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Main Authors: Sheykhi, Ahmad, Sooraki, Ava Shahbazi
Format: Preprint
Published: 2024
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author Sheykhi, Ahmad
Sooraki, Ava Shahbazi
author_facet Sheykhi, Ahmad
Sooraki, Ava Shahbazi
contents Using thermodynamics-gravity conjecture, we present the formal derivation of the modified Friedmann equations inspired by the Barrow entropy, $S\sim A ^{1+δ/2}$, where $0\leqδ\leq 1$ is the Barrow exponent and $A$ is the horizon area. We then constrain the exponent $δ$ by using Big-Bang Nucleosynthesis (BBN) observational data. In order to impose the upper bound on the Barrow exponent $δ$, we set the observational bound on $\left| \frac{δT_f} {T_f }\right|$. We find out that the Barrow parameter $δ$ should be around $ δ\simeq 0.01$ in order not to spoil the BBN era. Next we derive the bound on the Barrow exponent $δ$ in a different approach in which we analyze the effects of Barrow cosmology on the primordial abundances of light elements i.e. Helium $_{}^{4}\textit{He}$, Deuterium $D$ and Lithium $_{}^{7}\textit{Li}$. We observe that the deviation from standard Bekenstein-Hawking expression is small as expected. Additionally we present the relation between cosmic time $t$ and temperature $T$ in the context of modified Barrow cosmology. We confirm that the temperature of the early universe increases as the Barrow exponent $δ$ (fractal structure of the horizon) increases, too.
format Preprint
id arxiv_https___arxiv_org_abs_2411_06075
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Barrow Cosmology and Big-Bang Nucleosynthesis
Sheykhi, Ahmad
Sooraki, Ava Shahbazi
General Relativity and Quantum Cosmology
High Energy Physics - Theory
Using thermodynamics-gravity conjecture, we present the formal derivation of the modified Friedmann equations inspired by the Barrow entropy, $S\sim A ^{1+δ/2}$, where $0\leqδ\leq 1$ is the Barrow exponent and $A$ is the horizon area. We then constrain the exponent $δ$ by using Big-Bang Nucleosynthesis (BBN) observational data. In order to impose the upper bound on the Barrow exponent $δ$, we set the observational bound on $\left| \frac{δT_f} {T_f }\right|$. We find out that the Barrow parameter $δ$ should be around $ δ\simeq 0.01$ in order not to spoil the BBN era. Next we derive the bound on the Barrow exponent $δ$ in a different approach in which we analyze the effects of Barrow cosmology on the primordial abundances of light elements i.e. Helium $_{}^{4}\textit{He}$, Deuterium $D$ and Lithium $_{}^{7}\textit{Li}$. We observe that the deviation from standard Bekenstein-Hawking expression is small as expected. Additionally we present the relation between cosmic time $t$ and temperature $T$ in the context of modified Barrow cosmology. We confirm that the temperature of the early universe increases as the Barrow exponent $δ$ (fractal structure of the horizon) increases, too.
title Barrow Cosmology and Big-Bang Nucleosynthesis
topic General Relativity and Quantum Cosmology
High Energy Physics - Theory
url https://arxiv.org/abs/2411.06075