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dc.contributor.author | Zaslavskii O.B. | |
dc.date.accessioned | 2021-02-25T20:34:34Z | |
dc.date.available | 2021-02-25T20:34:34Z | |
dc.date.issued | 2020 | |
dc.identifier.issn | 0217-7323 | |
dc.identifier.uri | https://dspace.kpfu.ru/xmlui/handle/net/161798 | |
dc.description.abstract | © 2020 World Scientific Publishing Company. We consider collision of two particles 1 and 2 near the horizon of the extremal Reissner-Nordström (RN) black hole that produces two other particles 3 and 4. There exists such a scenario that both new particles fall into a black hole. One of them emerges from the white hole horizon in the asymptotically flat region, and the other one oscillates between turning points. However, the unbounded energies E at infinity (super-Penrose process (SPP)) turn out to be impossible for any finite angular momenta L3,4. In this sense, the situation for such a white hole scenarios is opposite to the black hole ones, where the SPP is found earlier to be possible for the RN metric even for all Li = 0. However, if L3,4 themselves are unbounded, the SPP does exist for white holes. | |
dc.relation.ispartofseries | Modern Physics Letters A | |
dc.subject | Particle collision | |
dc.subject | super-Penrose process | |
dc.subject | white holes | |
dc.title | Super-Penrose process for extremal charged white holes | |
dc.type | Article | |
dc.collection | Публикации сотрудников КФУ | |
dc.source.id | SCOPUS02177323-2020-SID85097904624 |