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May 7, 2026The European Physical Journal C0 citationsOpen Access

Dyonic Kerr–Sen black hole’s resonant scattering: absorption and superradiance

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SKSupakorn KatewongveerachartDSDavid Senjaya

Key Points

  • This research aims to analyze scalar superradiant scattering in the dyonic Kerr–Sen black hole.
  • Analytical investigation using the separable Klein–Gordon equation
  • Employing analytical asymptotic matching (AAM) method
  • Calculating reflection coefficient and superradiant amplification factor
  • Energy extraction occurs for co-rotating modes only
  • Electromagnetic charges suppress amplification compared to Kerr limit
  • Lighter co-rotating scalar fields enhance efficiency of rotational energy extraction

Abstract

Abstract We analytically investigate scalar superradiant scattering in the rotating dyonic Kerr–Sen black hole of Einstein–Maxwell-dilaton–axion theory. Starting from the separable Klein–Gordon equation for a massive neutral scalar field, we work in the low-frequency and slow-rotation regime and employ the analytical asymptotic matching (AAM) method to compute the reflection coefficient and the associated superradiant amplification factor. Since an exact global scattering solution is not available in this four-charge geometry, the AAM framework enables a controlled analytic treatment of the near-and far-region dynamics. We provide detailed and systematic derivations of the matching procedure leading to the closed-form amplification formula. The superradiant condition is obtained explicitly and we demonstrate that energy extraction occurs exclusively for co-rotating modes satisfying Ω m Ω H. We show that the presence of electric and magnetic charges suppresses the amplification relative to the Kerr limit, whereas lighter co-rotating scalar fields broaden the superradiant window and enhance the efficiency of rotational energy extraction.

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Cite This Study

Katewongveerachart et al. (2026) studied this question.

synapsesocial.com/papers/69fbf004164b5133a91a436fhttps://doi.org/10.1140/epjc/s10052-026-15717-w
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