Abstract
A small deformation to the Schwarzschild metric controlled by four free parameters could be referred to as a nonspinning black hole solution in alternative theories of gravity. Since such a non-Schwarzschild metric can be changed into a Kerr-like black hole metric via a complex coordinate transformation, the recently proposed time-transformed, explicit symplectic integrators for the Kerr-type spacetimes are suitable for a Hamiltonian system describing the motion of charged particles around the non-Schwarzschild black hole surrounded with an external magnetic field. The obtained explicit symplectic methods are based on a time-transformed Hamiltonian split into seven parts, whose analytical solutions are explicit functions of new coordinate time. Numerical tests show that such explicit symplectic integrators for intermediate time steps perform well long-term when stabilizing Hamiltonian errors, regardless of regular or chaotic orbits. One of the explicit symplectic integrators with the techniques of Poincaré sections and fast Lyapunov indicators is applied to investigate the effects of the parameters, including the four free deformation parameters, on the orbital dynamical behavior. From the global phase-space structure, chaotic properties are typically strengthened under some circumstances, as the magnitude of the magnetic parameter or any one of the negative deformation parameters increases. However, they are weakened when the angular momentum or any one of the positive deformation parameters increases.
Highlights
A Schwarzschild solution describing a nonrotating black hole and a Kerr solution describing a rotating black hole are two exact solutions of Einstein’s field equations of general relativity in a vacuum
There is the question of whether the time-transformed explicit symplectic integrators for the Kerr-type spacetimes [83] are applicable to such a deformed non-Schwarzschild black hole immersed in an external magnetic field
Such small deformation perturbations in the Schwarzschild metric could be regarded as a nonrotating black hole solution departure from the standard Schwarzschild spacetime in modified theories of gravity
Summary
A Schwarzschild solution describing a nonrotating black hole and a Kerr solution describing a rotating black hole are two exact solutions of Einstein’s field equations of general relativity in a vacuum. Thanks to the importance of the deformed (or modified) black hole solutions in tests of strong-field gravity features of general relativity, the motions of charged particles in the modified solutions with or without perturbations of weak external sources are naturally taken into account by some authors. Numerical integration methods are vital to detecting the chaotic behavior of charged particles in the vicinity of the standard general-relativistic or modified black hole solutions with or without perturbations from weak external sources. There is the question of whether the time-transformed explicit symplectic integrators for the Kerr-type spacetimes [83] are applicable to such a deformed non-Schwarzschild black hole immersed in an external magnetic field.
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