{"title":"GW170817后引力波对Palatini-Horndeski理论的约束","authors":"Yu-Qi Dong, Yu-Qiang Liu, Yu-Xiao Liu","doi":"10.1140/epjc/s10052-023-11861-9","DOIUrl":null,"url":null,"abstract":"<div><p>In this paper, we investigate the possible parameter space of Palatini–Horndeski theory with gravitational waves in a spatially flat Universe. We develop a general method for obtaining the speed of gravitational waves in the Palatini formalism in the cosmological background and we find that if the theory satisfies the following condition: in any spatially flat cosmological background, the tensor gravitational wave speed is the speed of light <i>c</i>, then only <span>\\(S = \\int d^4x \\sqrt{-g} \\big [K(\\phi ,X)-G_{3}(\\phi ,X){{\\tilde{\\Box }}}\\phi +G_{4}(\\phi ){\\tilde{R}}\\big ]\\)</span> is left as the possible action in Palatini–Horndeski theory. We also find that when <span>\\(G_{5}(\\phi ,X)\\ne 0\\)</span>, the tensor part of the connection will propagate and there are two different tensor gravitational wave speeds.</p></div>","PeriodicalId":788,"journal":{"name":"The European Physical Journal C","volume":"83 8","pages":""},"PeriodicalIF":4.2000,"publicationDate":"2023-08-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjc/s10052-023-11861-9.pdf","citationCount":"2","resultStr":"{\"title\":\"Constraining Palatini–Horndeski theory with gravitational waves after GW170817\",\"authors\":\"Yu-Qi Dong, Yu-Qiang Liu, Yu-Xiao Liu\",\"doi\":\"10.1140/epjc/s10052-023-11861-9\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>In this paper, we investigate the possible parameter space of Palatini–Horndeski theory with gravitational waves in a spatially flat Universe. We develop a general method for obtaining the speed of gravitational waves in the Palatini formalism in the cosmological background and we find that if the theory satisfies the following condition: in any spatially flat cosmological background, the tensor gravitational wave speed is the speed of light <i>c</i>, then only <span>\\\\(S = \\\\int d^4x \\\\sqrt{-g} \\\\big [K(\\\\phi ,X)-G_{3}(\\\\phi ,X){{\\\\tilde{\\\\Box }}}\\\\phi +G_{4}(\\\\phi ){\\\\tilde{R}}\\\\big ]\\\\)</span> is left as the possible action in Palatini–Horndeski theory. We also find that when <span>\\\\(G_{5}(\\\\phi ,X)\\\\ne 0\\\\)</span>, the tensor part of the connection will propagate and there are two different tensor gravitational wave speeds.</p></div>\",\"PeriodicalId\":788,\"journal\":{\"name\":\"The European Physical Journal C\",\"volume\":\"83 8\",\"pages\":\"\"},\"PeriodicalIF\":4.2000,\"publicationDate\":\"2023-08-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1140/epjc/s10052-023-11861-9.pdf\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The European Physical Journal C\",\"FirstCategoryId\":\"4\",\"ListUrlMain\":\"https://link.springer.com/article/10.1140/epjc/s10052-023-11861-9\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal C","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epjc/s10052-023-11861-9","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
Constraining Palatini–Horndeski theory with gravitational waves after GW170817
In this paper, we investigate the possible parameter space of Palatini–Horndeski theory with gravitational waves in a spatially flat Universe. We develop a general method for obtaining the speed of gravitational waves in the Palatini formalism in the cosmological background and we find that if the theory satisfies the following condition: in any spatially flat cosmological background, the tensor gravitational wave speed is the speed of light c, then only \(S = \int d^4x \sqrt{-g} \big [K(\phi ,X)-G_{3}(\phi ,X){{\tilde{\Box }}}\phi +G_{4}(\phi ){\tilde{R}}\big ]\) is left as the possible action in Palatini–Horndeski theory. We also find that when \(G_{5}(\phi ,X)\ne 0\), the tensor part of the connection will propagate and there are two different tensor gravitational wave speeds.
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