Causality in the maximally extended Reissner--Nordström spacetime with identifications

Andrzej Krasiński
{"title":"Causality in the maximally extended Reissner--Nordström spacetime with identifications","authors":"Andrzej Krasiński","doi":"arxiv-2409.03786","DOIUrl":null,"url":null,"abstract":"The maximally extended Reissner--Nordstr\\\"{o}m (RN) spacetime with $e^2 <\nm^2$ can be interpreted either as an infinite chain of asymptotically flat\nregions connected by tunnels between timelike singularities or as a set of just\none asymptotically flat region and one tunnel; the repetitions of this set in\nthe infinite chain being identified. The second interpretation gives rise to\nthe suspicion of acausality, i.e. the possibility of sending messages to one's\nown past. A numerical investigation of this problem was carried out in this\npaper and gave the following result. Let E be the initial point of a radial\ntimelike future-directed ingoing geodesic G, lying halfway between the outer\nhorizon and the image of the null infinity in the maximally extended RN\nspacetime. Let E$'$ be the first future copy of E. It was verified whether the\nturning point of G will lie to the future or to the past from the past light\ncone (PLC) of E$'$. In the second case the breach of causality does occur. It\nturned out that the acausality is present when $V_E$, the timelike coordinate\nof E, is negative with a sufficiently large $|V_E|$, and is absent with a\nsufficiently large $V_E > 0$. In between these values there exists a\n$\\widetilde{V}_E$, dependent on the initial data for the geodesic, for which\nthe turning point lies on the PLC. So, the identification does lead to\nacausality. Nonradial timelike and null geodesics were also investigated, and a\nfew hitherto unknown properties of the maximal extension were revealed. For\nexample, the singularity arc at $r = 0$ may be convex or concave, depending on\nthe values of $m$ and $e$.","PeriodicalId":501190,"journal":{"name":"arXiv - PHYS - General Physics","volume":"5 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - General Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.03786","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

The maximally extended Reissner--Nordstr\"{o}m (RN) spacetime with $e^2 < m^2$ can be interpreted either as an infinite chain of asymptotically flat regions connected by tunnels between timelike singularities or as a set of just one asymptotically flat region and one tunnel; the repetitions of this set in the infinite chain being identified. The second interpretation gives rise to the suspicion of acausality, i.e. the possibility of sending messages to one's own past. A numerical investigation of this problem was carried out in this paper and gave the following result. Let E be the initial point of a radial timelike future-directed ingoing geodesic G, lying halfway between the outer horizon and the image of the null infinity in the maximally extended RN spacetime. Let E$'$ be the first future copy of E. It was verified whether the turning point of G will lie to the future or to the past from the past light cone (PLC) of E$'$. In the second case the breach of causality does occur. It turned out that the acausality is present when $V_E$, the timelike coordinate of E, is negative with a sufficiently large $|V_E|$, and is absent with a sufficiently large $V_E > 0$. In between these values there exists a $\widetilde{V}_E$, dependent on the initial data for the geodesic, for which the turning point lies on the PLC. So, the identification does lead to acausality. Nonradial timelike and null geodesics were also investigated, and a few hitherto unknown properties of the maximal extension were revealed. For example, the singularity arc at $r = 0$ may be convex or concave, depending on the values of $m$ and $e$.
最大扩展赖斯纳--诺德斯特伦时空中的因果性与识别性
Reissner--Nordstr\"{o}m (RN)时空的最大扩展值为$e^2 0$。在这两个值之间存在一个取决于测地线初始数据的$widetilde{V}_E$,其转折点位于PLC上。因此,这种辨别确实会导致谬误。我们还研究了非径向时间线和空大地线,并揭示了最大延伸线迄今未知的一些特性。例如,在 $r = 0$ 处的奇点弧可能是凸的,也可能是凹的,这取决于 $m$ 和 $e$ 的值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信