2022
DOI: 10.1140/epjc/s10052-022-10560-1
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Constraints on the magnetized Ernst black hole spacetime through quasiperiodic oscillations

Abstract: We study the dynamics of test particles around a magnetized Ernst black hole considering its magnetic field in the environment surrounding the black hole. We show how its magnetic field can influence the dynamics of particles and epicyclic motion around the black hole. Based on the analysis, we find that the radius of the innermost stable circular orbit (ISCO) for both neutral and charged test particles and epicyclic frequencies are strongly affected by the influence of the magnetic field. We also show that th… Show more

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Cited by 22 publications
(6 citation statements)
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“…If the value of B increases from 0 to M −1 and more, the ISCO radius decreases from 6M to 2M and then disappears behind the horizon. For weak magnetic field, i.e., B << M −1 , the ISCO occurs close to 6M but the exact value is lower than 6M [20]. Now, in this respect, we recall that the parameter r B in our spacetime metric is roughly the extent of the region over which the magnetic field a uniform.…”
Section: B Innermost Stable Circular Orbit In the Ems Black Holementioning
confidence: 92%
“…If the value of B increases from 0 to M −1 and more, the ISCO radius decreases from 6M to 2M and then disappears behind the horizon. For weak magnetic field, i.e., B << M −1 , the ISCO occurs close to 6M but the exact value is lower than 6M [20]. Now, in this respect, we recall that the parameter r B in our spacetime metric is roughly the extent of the region over which the magnetic field a uniform.…”
Section: B Innermost Stable Circular Orbit In the Ems Black Holementioning
confidence: 92%
“…We demonstrate how its magnetic field can affect the Hawking radiation. The fourdimensional Ernst metric [64,65] has the following form…”
Section: Hawking Radiation From Magnetised Ernst-like Black Holementioning
confidence: 99%
“…Here, ν r and ν θ are the frequencies of the perturbed circular motion as detected by an observer at spatial infinity, which are related to the local frequencies, Ω r and Ω θ , by ν r = Ω r /(2πu t ) and ν θ = Ω θ /(2πu t ), where u t and u j are the only nonvanishing components of the four-velocity vector of the infalling particle. Expressions similar to Equations (69) and (70) in the presence of a magnetic source were derived in Shaymatov et al (2022).…”
Section: Limits On the Parameters Of Prz Spacetime Via Quasiperiodic ...mentioning
confidence: 99%