Can Power-Law Entropic Corrections Account for the Baryon Asymmetry in the Early Universe?

IF 5 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS
Kalyan Malakar, Mrinnoy M. Gohain, Kalyan Bhuyan
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引用次数: 0

Abstract

The origin of the observed baryon imbalance of Universe remains an unresolved problem in modern cosmology. In this work, we investigate whether baryon asymmetry can be realized in the presence of power-law corrections to horizon entropy motivated by quantum entanglement. Within the emergent-spacetime framework, we derive the modified Friedmann and Raychaudhuri equations and implement a perturbative expansion around the radiation-dominated background. We demonstrate that the entropy correction results in a nonzero curvature scalar (R) and its time derivative, thereby enabling the generation of baryon asymmetry in a regime where the standard scenario yields no asymmetry. We calculate the baryon number to entropy ratio arising from the curvature-current interaction and constrain the model parameters using observational bounds. The measured baryon excess is reproduced for the value (α ≃ 1.974) of the entropy correction quantity, demonstrating that entropic modifications to cosmological dynamics provide a viable and geometrically motivated mechanism for baryogenesis. This result highlights that even minute entanglement-induced corrections can leave observable imprints on early-universe dynamics.
幂律熵修正能解释早期宇宙中的重子不对称性吗?
在现代宇宙学中,观测到的宇宙重子不平衡的起源仍然是一个未解决的问题。在这项工作中,我们研究了重子不对称是否可以在由量子纠缠引起的视界熵幂律修正存在的情况下实现。在紧急时空框架内,我们推导了修正的Friedmann和Raychaudhuri方程,并实现了围绕辐射主导背景的微扰展开。我们证明了熵修正导致非零曲率标量(R)及其时间导数,从而使在标准场景不产生不对称的情况下产生重子不对称。我们计算了由曲率-电流相互作用引起的重子数与熵比,并利用观测界对模型参数进行了约束。在熵修正量(α ≃ 1.974)处再现了测量到的重子过量,表明宇宙学动力学的熵修正为重子发生提供了一种可行的几何激励机制。这个结果强调,即使是微小的纠缠引起的修正也会在早期宇宙动力学上留下可观察到的印记。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Physics Letters B
Physics Letters B 物理-物理:综合
CiteScore
9.10
自引率
6.80%
发文量
647
审稿时长
3 months
期刊介绍: Physics Letters B ensures the rapid publication of important new results in particle physics, nuclear physics and cosmology. Specialized editors are responsible for contributions in experimental nuclear physics, theoretical nuclear physics, experimental high-energy physics, theoretical high-energy physics, and astrophysics.
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