{"title":"黑洞的黑域观测器","authors":"Theodorus Maria Nieuwenhuizen","doi":"arxiv-2405.19560","DOIUrl":null,"url":null,"abstract":"A class of observers is introduced that interpolate smoothly between the\nSchwarzschild observer, stable at spatial infinity, and the Kerr-Schild\nobserver, who falls into a black hole. For these observers the passing of the\nevent and inner horizon takes a finite time, which diverges logarithmically\nwhen the interpolation parameter $\\sigma$ goes to zero. In the field theoretic\napproach to gravitation, the behavior at the horizons becomes regular, making\nthe mass of the metric well defined.","PeriodicalId":501190,"journal":{"name":"arXiv - PHYS - General Physics","volume":"17 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-05-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The smeared-horizon observer of a black hole\",\"authors\":\"Theodorus Maria Nieuwenhuizen\",\"doi\":\"arxiv-2405.19560\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A class of observers is introduced that interpolate smoothly between the\\nSchwarzschild observer, stable at spatial infinity, and the Kerr-Schild\\nobserver, who falls into a black hole. For these observers the passing of the\\nevent and inner horizon takes a finite time, which diverges logarithmically\\nwhen the interpolation parameter $\\\\sigma$ goes to zero. In the field theoretic\\napproach to gravitation, the behavior at the horizons becomes regular, making\\nthe mass of the metric well defined.\",\"PeriodicalId\":501190,\"journal\":{\"name\":\"arXiv - PHYS - General Physics\",\"volume\":\"17 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-05-29\",\"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-2405.19560\",\"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 - General Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2405.19560","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A class of observers is introduced that interpolate smoothly between the
Schwarzschild observer, stable at spatial infinity, and the Kerr-Schild
observer, who falls into a black hole. For these observers the passing of the
event and inner horizon takes a finite time, which diverges logarithmically
when the interpolation parameter $\sigma$ goes to zero. In the field theoretic
approach to gravitation, the behavior at the horizons becomes regular, making
the mass of the metric well defined.