2021
DOI: 10.1140/epjc/s10052-021-09933-9
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Absorption by stringy black holes

Abstract: We investigate the absorption of planar massless scalar waves by a charged rotating stringy black hole, namely a Kerr–Sen black hole. We compute numerically the absorption cross section and compare our results with those of the Kerr–Newman black hole, a classical general relativity solution. In order to better compare both charged black holes, we define the ratio of the black hole charge to the extreme charge as Q. We conclude that Kerr–Sen and Kerr–Newman black holes have a similar absorption cross section, w… Show more

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Cited by 6 publications
(2 citation statements)
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“…( 94) and angular velocity is Ω ph with the radius of the photon sphere r ph . Hence, the Sinc approximation said that the total absorption cross section at the eikonal limit is σ abs ≈ σ osc +σ geo [123,[125][126][127][128][129][130]. In the Fig.…”
Section: Bounds Of Greybody Factors and High-energy Absorption Cross-...mentioning
confidence: 99%
“…( 94) and angular velocity is Ω ph with the radius of the photon sphere r ph . Hence, the Sinc approximation said that the total absorption cross section at the eikonal limit is σ abs ≈ σ osc +σ geo [123,[125][126][127][128][129][130]. In the Fig.…”
Section: Bounds Of Greybody Factors and High-energy Absorption Cross-...mentioning
confidence: 99%
“…x ) with the photon sphere. This method extensively discussed in the literature [197][198][199][200][201][202][203]. In the limit of high energy, the oscillatory part of the absorption cross-section can be calculated by using [144]:…”
Section: Bounds Of Greybody Factors and High-energy Absorption Cross-...mentioning
confidence: 99%