dc.contributor.author |
Zaslavskii O.B. |
|
dc.date.accessioned |
2021-02-26T20:51:01Z |
|
dc.date.available |
2021-02-26T20:51:01Z |
|
dc.date.issued |
2020 |
|
dc.identifier.issn |
2470-0010 |
|
dc.identifier.uri |
https://dspace.kpfu.ru/xmlui/handle/net/163242 |
|
dc.description.abstract |
© 2020 American Physical Society. We consider particle collisions in the background of a nonextremal black hole. Two particles fall from infinity, particle 1 is fine-tuned (critical), collision occurs in its turning point. The first example is the Reissner-Nordström (RN) one. If the energy at infinity E1 is big enough, the turning point is close to the horizon. Then, we derive a simple formula according to which Ec.m.~E1?-1/2, where ? is a surface gravity. Thus significant growth of Ec.m. is possible if (i) particle 1 is ultrarelativistic (if both particles are ultrarelativistic, this gives no gain as compared to collisions in flat space-time), (ii) a black hole is near-extremal (small ?). In the scenario of multiple collisions the energy Ec.m. is finite in each individual collision. However, it can grow in subsequent collisions, provided new near-critical particles are heavy enough. For neutral rotating black holes, in case (i) a turning point remains far from the horizon but large Ec.m. is still possible. Case (ii) is similar to that for collisions in the RN metric. We develop a general theoretical scheme, direct astrophysical applications can be a next step to be studied. |
|
dc.relation.ispartofseries |
Physical Review D |
|
dc.title |
Can a nonextremal black hole be a particle accelerator |
|
dc.type |
Article |
|
dc.relation.ispartofseries-issue |
10 |
|
dc.relation.ispartofseries-volume |
102 |
|
dc.collection |
Публикации сотрудников КФУ |
|
dc.source.id |
SCOPUS24700010-2020-102-10-SID85096083716 |
|