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    Characteristic initial value problems for the Einstein-Maxwell-scalar field equations in spherical symmetry

    Thomas Mädler*

    Radouane Gannouji†

    Emanuel Gallo‡

    • Escuela de Obras Civiles and Instituto de Estudios Astrofísicos, Facultad de Ingeniería y Ciencias, Universidad Diego Portales, Avenida Ejército Libertador 441, Casilla 298-V, Santiago, Chile

    • Universidad Nacional de Córdoba, Facultad de Matemática, Astronomía, Física y Computación, Grupo de Relatividad y Gravitación, Córdoba, Argentina and Consejo Nacional de Investigaciones Científicas y Técnicas, CONICET, IFEG, Córdoba, Argentina

    • *Contact author: thomas.maedler@mail.udp.cl
    • †Contact author: radouane.gannouji@pucv.cl
    • ‡Contact author: egallo@unc.edu.ar

    Phys. Rev. D 111, 124015 – Published 11 June, 2025

    DOI: https://doi.org/10.1103/f5fc-zpld

    Abstract

    The characteristic initial boundary problem is discussed in spherical symmetry for the Einstein-Maxwell-scalar field equations. It is formulated for an affine-null metric, and the resulting field equations are cast into a hierarchical system of partial differential equations. The initial boundary value problem for a family of null hypersurfaces is specified for a timelike-null foliation at the central geodesic of spherical symmetry as well as for a double-null foliation where the corresponding boundary is a null hypersurface. For the latter, two distinct boundary value formulations arise: one where the null boundary has zero Misner-Sharp mass, and another one where the corresponding Misner-Sharp mass is nonzero. As an application, the nonextremal and the extremal Reissner-Nordström solution in null coordinates for a charged black hole and the Fisher-Janis-Newman-Winicour solution are derived.

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