{"title":"Flat subspaces of the \\(SL(n,\\mathbb {R})\\) chiral equations","authors":"I. A. Sarmiento-Alvarado, P. Wiederhold, T. Matos","doi":"10.1007/s10714-025-03467-1","DOIUrl":null,"url":null,"abstract":"<div><p>In this work, we introduce a method for finding exact solutions to the vacuum Einstein field equations in higher dimensions from a given solution to the chiral equation. When considering a <span>\\(n + 2\\)</span>-dimensional spacetime with <i>n</i> commutative Killing vectors, the metric tensor can take the form <span>\\(\\hat{g} = f ( \\rho , \\zeta ) ( d \\rho ^2 + d \\zeta ^2 ) + g_{\\mu \\nu } ( \\rho , \\zeta ) d x^\\mu d x^\\nu \\)</span>. Then, the Einstein field equations in vacuum reduce to a chiral equation, <span>\\(( \\rho g_{, z} g ^{-1} )_{, \\bar{z}} + ( \\rho g_{, \\bar{z}} g ^{-1} )_{, z} = 0\\)</span>, and two differential equations, <span>\\(( \\ln f \\rho ^{1-1/n} )_{, Z} = \\frac{\\rho }{2} \\operatorname {tr} ( g_{, _Z} g^{-1} )^2\\)</span>, where <span>\\(g \\in SL( n, \\mathbb {R} )\\)</span> is the normalized matrix representation of <span>\\(g_{\\mu \\nu }\\)</span>, <span>\\(z = \\rho + i \\zeta \\)</span> and <span>\\(Z = z, \\bar{z}\\)</span>. We use the ansatz <span>\\(g = g ( \\xi ^a )\\)</span>, where the parameters <span>\\(\\xi ^a\\)</span> depend on <i>z</i> and <span>\\(\\bar{z}\\)</span> and satisfy a generalized Laplace equation, <span>\\(( \\rho \\xi ^a _{, z} )_{, \\bar{z}} + ( \\rho \\xi ^a _{, \\bar{z}} )_{, z} = 0\\)</span>. The chiral equation to the Killing equation, <span>\\(A_{a, \\xi ^b} + A_{b, \\xi ^a} = 0\\)</span>, where <span>\\(A_a = g_{, \\xi ^a} g^{-1}\\)</span>. Furthermore, we assume that the matrices <span>\\(A_a\\)</span> commute with each other; in this way, they fulfill the Killing equation.</p></div>","PeriodicalId":578,"journal":{"name":"General Relativity and Gravitation","volume":"57 9","pages":""},"PeriodicalIF":2.8000,"publicationDate":"2025-09-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10714-025-03467-1.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"General Relativity and Gravitation","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s10714-025-03467-1","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
引用次数: 0
Abstract
In this work, we introduce a method for finding exact solutions to the vacuum Einstein field equations in higher dimensions from a given solution to the chiral equation. When considering a \(n + 2\)-dimensional spacetime with n commutative Killing vectors, the metric tensor can take the form \(\hat{g} = f ( \rho , \zeta ) ( d \rho ^2 + d \zeta ^2 ) + g_{\mu \nu } ( \rho , \zeta ) d x^\mu d x^\nu \). Then, the Einstein field equations in vacuum reduce to a chiral equation, \(( \rho g_{, z} g ^{-1} )_{, \bar{z}} + ( \rho g_{, \bar{z}} g ^{-1} )_{, z} = 0\), and two differential equations, \(( \ln f \rho ^{1-1/n} )_{, Z} = \frac{\rho }{2} \operatorname {tr} ( g_{, _Z} g^{-1} )^2\), where \(g \in SL( n, \mathbb {R} )\) is the normalized matrix representation of \(g_{\mu \nu }\), \(z = \rho + i \zeta \) and \(Z = z, \bar{z}\). We use the ansatz \(g = g ( \xi ^a )\), where the parameters \(\xi ^a\) depend on z and \(\bar{z}\) and satisfy a generalized Laplace equation, \(( \rho \xi ^a _{, z} )_{, \bar{z}} + ( \rho \xi ^a _{, \bar{z}} )_{, z} = 0\). The chiral equation to the Killing equation, \(A_{a, \xi ^b} + A_{b, \xi ^a} = 0\), where \(A_a = g_{, \xi ^a} g^{-1}\). Furthermore, we assume that the matrices \(A_a\) commute with each other; in this way, they fulfill the Killing equation.
期刊介绍:
General Relativity and Gravitation is a journal devoted to all aspects of modern gravitational science, and published under the auspices of the International Society on General Relativity and Gravitation.
It welcomes in particular original articles on the following topics of current research:
Analytical general relativity, including its interface with geometrical analysis
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Gravitational waves: data analysis, astrophysical sources and detector science
Extensions of general relativity
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Gravitational aspects of string theory and its extensions
Quantum gravity: canonical approaches, in particular loop quantum gravity, and path integral approaches, in particular spin foams, Regge calculus and dynamical triangulations
Quantum field theory in curved spacetime
Non-commutative geometry and gravitation
Experimental gravity, in particular tests of general relativity
The journal publishes articles on all theoretical and experimental aspects of modern general relativity and gravitation, as well as book reviews and historical articles of special interest.