2014
DOI: 10.1007/jhep03(2014)113
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Bounding the greybody factors for scalar field excitations on the Kerr-Newman spacetime

Abstract: Finding exact solutions for black-hole greybody factors is generically impractical; typically one resorts either to making semi-analytic or numerical estimates, or alternatively to deriving rigorous analytic bounds. Indeed, rigorous bounds have already been established for the greybody factors of Schwarzschild and Riessner-Nordström black holes, and more generally for those of arbitrary static spherically symmetric asymptotically flat black holes. Adding rotation to the problem greatly increases the level of d… Show more

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Cited by 34 publications
(37 citation statements)
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“…(29) Note that the equivalent result for n = 0 was already derived in Ref. 11 for the Kerr-Newman spacetime. Second, for n ≥ 0, we also have n(n − 2) (r ) 4r 2 + n (r ) 2r ∝ n{(n − 2) (r ) + 2r (r )} = n{(n + 2)r 2 + (n − 2)a 2 + nμr 1−n }.…”
Section: Positivity Propertiesmentioning
confidence: 61%
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“…(29) Note that the equivalent result for n = 0 was already derived in Ref. 11 for the Kerr-Newman spacetime. Second, for n ≥ 0, we also have n(n − 2) (r ) 4r 2 + n (r ) 2r ∝ n{(n − 2) (r ) + 2r (r )} = n{(n + 2)r 2 + (n − 2)a 2 + nμr 1−n }.…”
Section: Positivity Propertiesmentioning
confidence: 61%
“…Furthermore, the separation constant and effective potential reduce to those discussed in Ref. 11. Ultimately, the bounds on the greybody factors reduce (as they should) to those of Ref.…”
Section: B Highly Super-radiant Modes (M ≥ 2m * )mentioning
confidence: 77%
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