{"title":"Effective Pressure of the FRW Universe","authors":"Shi-Bei Kong","doi":"10.1016/j.aop.2025.170163","DOIUrl":null,"url":null,"abstract":"<div><div>In this paper, we study the effective pressure of the <span><math><mi>N</mi></math></span>-dimensional FRW(Friedmann–Robertson– Walker) universe in Einstein gravity, Gauss–Bonnet gravity, and Lovelock gravity. The effective pressure is defined by <span><math><mrow><msub><mrow><mi>P</mi></mrow><mrow><mi>e</mi><mi>f</mi><mi>f</mi></mrow></msub><mo>≔</mo><mo>−</mo><mi>d</mi><mi>E</mi><mo>/</mo><mi>d</mi><mi>V</mi></mrow></math></span>, where <span><math><mrow><mi>E</mi><mo>=</mo><mi>ρ</mi><mi>V</mi></mrow></math></span> is the effective energy and <span><math><mi>V</mi></math></span> is the volume of the FRW universe inside the apparent horizon. The effective pressure in Einstein gravity is always negative and its absolute value decreases with the horizon radius <span><math><msub><mrow><mi>R</mi></mrow><mrow><mi>A</mi></mrow></msub></math></span>. The effective pressure in Gauss–Bonnet gravity is different with the one in Einstein gravity only when <span><math><mrow><mi>N</mi><mo>≥</mo><mn>6</mn></mrow></math></span>, and in this case, the effective pressure is not always negative and has a minimum, which is very similar to the potential between molecules. The effective pressure in Lovelock gravity can have multiple zero-points and extreme points. The effective pressure in different dimensions has interesting relations. We also find that under certain condition, the effective pressure is equivalent with the ‘ordinary’ pressure <span><math><mi>p</mi></math></span> of the perfect fluid, and this condition do not depend on the specific choice of gravitational theories.</div></div>","PeriodicalId":8249,"journal":{"name":"Annals of Physics","volume":"481 ","pages":"Article 170163"},"PeriodicalIF":3.0000,"publicationDate":"2025-07-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Annals of Physics","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0003491625002453","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
In this paper, we study the effective pressure of the -dimensional FRW(Friedmann–Robertson– Walker) universe in Einstein gravity, Gauss–Bonnet gravity, and Lovelock gravity. The effective pressure is defined by , where is the effective energy and is the volume of the FRW universe inside the apparent horizon. The effective pressure in Einstein gravity is always negative and its absolute value decreases with the horizon radius . The effective pressure in Gauss–Bonnet gravity is different with the one in Einstein gravity only when , and in this case, the effective pressure is not always negative and has a minimum, which is very similar to the potential between molecules. The effective pressure in Lovelock gravity can have multiple zero-points and extreme points. The effective pressure in different dimensions has interesting relations. We also find that under certain condition, the effective pressure is equivalent with the ‘ordinary’ pressure of the perfect fluid, and this condition do not depend on the specific choice of gravitational theories.
期刊介绍:
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