{"title":"黑洞和玻色子星的广义科马尔电荷和斯马尔公式","authors":"Romina Ballesteros, Tomas Ortin","doi":"arxiv-2409.08268","DOIUrl":null,"url":null,"abstract":"The standard Komar charge is a $(d-2)$-form that can be defined in spacetimes\nadmitting a Killing vector and which is closed when the vacuum Einstein\nequations are satisfied. Its integral at spatial infinity (the Komar integral)\ngives the conserved charge associated to the Killing vector, and, due to its\non-shell closedness, the same value (expressed in terms of other physical\nvariables) is obtained integrating over the event horizon (if any). This\nequality is the basis of the Smarr formula. This charge can be generalized so\nthat it still is closed on-shell in presence of matter and its integrals give\ngeneralizations of the Smarr formula. We show how the Komar charge and other\nclosed $(d-2)$-form charges can be used to prove non-existence theorems for\ngravitational solitons and boson stars. In particular, we show how one can deal\nwith generalized symmetric fields (invariant under a combination of isometries\nand other global symmetries) and how the geralized symmetric ansatz permits to\nevade the non-existence theorems.","PeriodicalId":501339,"journal":{"name":"arXiv - PHYS - High Energy Physics - Theory","volume":"16 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Generalized Komar charges and Smarr formulas for black holes and boson stars\",\"authors\":\"Romina Ballesteros, Tomas Ortin\",\"doi\":\"arxiv-2409.08268\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The standard Komar charge is a $(d-2)$-form that can be defined in spacetimes\\nadmitting a Killing vector and which is closed when the vacuum Einstein\\nequations are satisfied. Its integral at spatial infinity (the Komar integral)\\ngives the conserved charge associated to the Killing vector, and, due to its\\non-shell closedness, the same value (expressed in terms of other physical\\nvariables) is obtained integrating over the event horizon (if any). This\\nequality is the basis of the Smarr formula. This charge can be generalized so\\nthat it still is closed on-shell in presence of matter and its integrals give\\ngeneralizations of the Smarr formula. We show how the Komar charge and other\\nclosed $(d-2)$-form charges can be used to prove non-existence theorems for\\ngravitational solitons and boson stars. In particular, we show how one can deal\\nwith generalized symmetric fields (invariant under a combination of isometries\\nand other global symmetries) and how the geralized symmetric ansatz permits to\\nevade the non-existence theorems.\",\"PeriodicalId\":501339,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Physics - Theory\",\"volume\":\"16 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-12\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Physics - Theory\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.08268\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.08268","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Generalized Komar charges and Smarr formulas for black holes and boson stars
The standard Komar charge is a $(d-2)$-form that can be defined in spacetimes
admitting a Killing vector and which is closed when the vacuum Einstein
equations are satisfied. Its integral at spatial infinity (the Komar integral)
gives the conserved charge associated to the Killing vector, and, due to its
on-shell closedness, the same value (expressed in terms of other physical
variables) is obtained integrating over the event horizon (if any). This
equality is the basis of the Smarr formula. This charge can be generalized so
that it still is closed on-shell in presence of matter and its integrals give
generalizations of the Smarr formula. We show how the Komar charge and other
closed $(d-2)$-form charges can be used to prove non-existence theorems for
gravitational solitons and boson stars. In particular, we show how one can deal
with generalized symmetric fields (invariant under a combination of isometries
and other global symmetries) and how the geralized symmetric ansatz permits to
evade the non-existence theorems.