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Black holes in nonlinear electrodynamics: Quasinormal spectra and parity splitting

Eliana ChaverraDepartamento de Física, División de Ciencias e Ingeniería, Campus León, Universidad de Guanajuato, 37150 León, MéxicoJuan Carlos DegolladoInstituto de Ciencias Físicas, Universidad Nacional Autónoma de México, Apartado Postal 48-3, 62251 Cuernavaca, Morelos, MéxicoClaudia MorenoDepartamento de Física, Centro Universitario de Ciencias Exactas e Ingenierías, Universidad de Guadalajara, Avenida Revolución 1500, Colonia Olímpica 44430 Guadalajara, Jalisco, MéxicoOlivier SarbachInstituto de Física y Matemáticas, Universidad Michoacana de San Nicolás de Hidalgo, Edificio C-3, Ciudad Universitaria, 58040 Morelia, Michoacán, México
2016en
ABI

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We discuss the quasinormal oscillations of black holes which are sourced by a nonlinear electrodynamic field. While previous studies have focused on the computation of quasinormal frequencies for the wave or higher spin equation on a fixed background geometry described by such black holes, here we compute for the first time the quasinormal frequencies for the coupled electromagnetic-gravitational linear perturbations. To this purpose, we consider a parametrized family of Lagrangians for the electromagnetic field which contains the Maxwell Lagrangian as a special case. In the Maxwell case, the unique spherically symmetric black hole solutions are described by the Reissner-Nordstr\"om family and in this case it is well known that the quasinormal spectra in the even- and odd-parity sectors are identical to each other. However, when moving away from the Maxwell case, we obtain deformed Reissner-Nordstr\"om black holes, and we show that in this case there is a parity splitting in the quasinormal mode spectra. A partial explanation for this phenomena is provided by considering the eikonal (high-frequency) limit.

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