- Open Access
Analytic computation of dilaton black hole quasinormal modes via the Seiberg-Witten theory
Phys. Rev. D 113, 046007 – Published 10 February, 2026
DOI: https://doi.org/10.1103/71pw-vxlw
Abstract
We study the quasinormal modes (QNMs) of dilaton black holes in Einstein-Maxwell-dilaton gravity through a correspondence with the quantum Seiberg-Witten (SW) curve of SU(2) gauge theory with hypermultiplets. By mapping both the black hole perturbation equation and the quantum SW curve to the confluent Heun form, the QNM problem is reformulated in a gauge-theoretic framework, and the spectrum is obtained via the SW quantization condition. The resulting frequencies show excellent agreement with those computed using the WKB and continued fraction methods, with typical deviations below . The QNM spectrum exhibits consistent trends: increasing the black hole charge or scalar field mass raises the oscillation frequency, while higher angular momentum reduces the damping rate. These results demonstrate the precision of the quantum SW framework in describing black hole perturbations and reveal new links between supersymmetric gauge theories and gravitational dynamics.
Physics Subject Headings (PhySH)
Article Text
References (31)
- B. P. Abbott et al. (LIGO Scientific and Virgo Collaborations), Phys. Rev. Lett. 116, 061102 (2016).
- G. W. Gibbons and K. i. Maeda, Nucl. Phys. B298, 741 (1988).
- D. Garfinkle, G. T. Horowitz, and A. Strominger, Phys. Rev. D 43, 3140 (1991); 45, 3888(E) (1992).
- Z. Malik, Int. J. Theor. Phys. 63, 128 (2024).
- R. A. Konoplya and A. Zhidenko, Phys. Rev. D 107, 044009 (2023).
- V. Ferrari, M. Pauri, and F. Piazza, Phys. Rev. D 63, 064009 (2001).
- R. Brito and C. Pacilio, Phys. Rev. D 98, 104042 (2018).
- C. N. Pope, D. O. Rohrer, and B. F. Whiting, Phys. Rev. D 110, 104036 (2024).
- N. Seiberg and E. Witten, Nucl. Phys. B426, 19 (1994); B430, 485(E) (1994).
- N. Seiberg and E. Witten, Nucl. Phys. B431, 484 (1994).
- G. Bonelli, C. Iossa, D. P. Lichtig, and A. Tanzini, Phys. Rev. D 105, 044047 (2022).
- G. Aminov, A. Grassi, and Y. Hatsuda, Ann. Henri Poincare 23, 1951 (2022).
- M. Bianchi, D. Consoli, A. Grillo, and J. F. Morales, J. High Energy Phys. 01 (2022) 024.
- X. H. Ge, M. Matsumoto, and K. Zhang, Phys. Rev. D 112, 046024 (2025).
- X. H. Ge, M. Matsumoto, and K. Zhang, J. High Energy Phys. 05 (2024) 336.
- H. O. Silva, J. W. Kim, and M. V. S. Saketh, Phys. Rev. D 111, 104021 (2025).
- Y. Lei, H. Shu, K. Zhang, and R. D. Zhu, J. High Energy Phys. 02 (2024) 140.
- B. F. Schutz and C. M. Will, Astrophys. J. Lett. 291, L33 (1985).
- S. Iyer and C. M. Will, Phys. Rev. D 35, 3621 (1987).
- R. A. Konoplya, Phys. Rev. D 68, 024018 (2003).
- J. Matyjasek and M. Opala, Phys. Rev. D 96, 024011 (2017).
- R. A. Konoplya, A. Zhidenko, and A. F. Zinhailo, Classical Quantum Gravity 36, 155002 (2019).
- E. W. Leaver, Proc. R. Soc. A 402, 285 (1985).
- R. A. Konoplya and A. Zhidenko, Rev. Mod. Phys. 83, 793 (2011).
- The Mathematica package with the WKB formula of 13th order and Padé approximations ready for calculation of the quasinormal modes and grey-body factors, as well as examples of such calculations for the Schwarzschild black hole are publicly available to download from https://goo.gl/nykYGL.
- M. Bianchi, D. Consoli, A. Grillo, and J. F. Morales, Phys. Lett. B 824, 136837 (2022).
- K. Imaizumi, Phys. Lett. B 834, 137450 (2022).
- K. Imaizumi, Nucl. Phys. B992, 116221 (2023).
- N. A. Nekrasov, Adv. Theor. Math. Phys. 7, 831 (2003).
- N. A. Nekrasov and S. L. Shatashvili, arXiv:0908.4052.
- M. Matone, Phys. Lett. B 357, 342 (1995).