In this work, we consider an extension of the symmetric teleparallel equivalent of General Relativity (STEGR), namely, f(Q) f ( Q ) gravity, by including a boundary term BQ B Q , where Q Q is the non-metricity scalar. More specifically, we explore static and spherically symmetric black hole and regular black hole solutions in f(Q,BQ) f ( Q , B Q ) gravity coupled to nonlinear electrodynamics (NLED). In particular, to obtain black hole solutions, and in order to ensure that our solutions preserve Lorentz symmetry, we assume the following relation fQ = -fB f Q = - f B , where fQ=∂ f/∂ Q f Q = ∂ f / ∂ Q and fB= ∂ f/∂ BQ f B = ∂ f / ∂ B Q . We develop three models of black holes, and as the starting point for each case we consider the non-metricity scalar or the boundary term in such a way to obtain the metric functions A ( r ). Additionally, we are able to express matter through analytical solutions for specific NLED Lagrangians LNLED(F) L NLED ( F ) . Furthermore, we also obtain generalized solutions of the Bardeen and Culetu types of regular black holes, by imposing specific metric functions.
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S. et al. (2024) studied this question.
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