2016
DOI: 10.1103/physrevd.94.044038
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Stable photon orbits in stationary axisymmetric electrovacuum spacetimes

Abstract: We investigate the existence and phenomenology of stable photon orbits (SPOs) in stationary axisymmetric electrovacuum spacetimes in four dimensions. First, we review the classification of equatorial circular photon orbits on Kerr-Newman spacetimes in the charge-spin plane. Second, using a Hamiltonian formulation, we show that Reissner-Nordström di-holes (a family encompassing the Majumdar-Papapetrou and Weyl-Bach special cases) admit SPOs, in a certain parameter regime that we investigate. Third, we explore t… Show more

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Cited by 30 publications
(27 citation statements)
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“…Above the minimum, the bounded light orbits with two radial turning points are located. Their existence serves an indication that the solution may be unstable [17][18][19][20]. Stable photon rings are often encountered near (hypothetical) horizonless ultra-compact objects, thus indicating on their instability [21].…”
Section: Introductionmentioning
confidence: 99%
“…Above the minimum, the bounded light orbits with two radial turning points are located. Their existence serves an indication that the solution may be unstable [17][18][19][20]. Stable photon rings are often encountered near (hypothetical) horizonless ultra-compact objects, thus indicating on their instability [21].…”
Section: Introductionmentioning
confidence: 99%
“…Thus, the equipotential lines of h AE ðr; θÞ give the boundary of the allowed region in the ðr; θÞ-space, for each value of η. A similar effective potential was recently used in [45,46]. Moreover, since the solutions of the quadratic equation are In the limit g tt → 0, one of the functions h AE diverges and the other converges toh.…”
Section: B the Two 2d Effective Potentialsmentioning
confidence: 99%
“…1. Chaotic scattering in GR spacetimes has been observed and discussed in binary or multi-BH solutions (see, e.g., [45,46,[74][75][76][77][78][79][80][81][82][83][84]) and is well known in the context of manybody scattering in classical dynamics, for example, the scattering of charged particles off magnetic dipoles [85] and the three-body problem (see, e.g., [86]). KBHsSH or RBSs provide an example of chaos in geodesic motion on the background of a single compact object, which moreover solves a simple and well-defined matter model minimally coupled to GR.…”
Section: Introductionmentioning
confidence: 99%
“…In addition, h 0 (ρ, 0) also vanishes for g = 0, which is similar to the behavior seen in Eqs. (25) and (26). This fact implies that the monotonicity of angular momentum and energy for a circular orbit switches at zeros of h 0 (ρ, 0).…”
Section: Stability Conditions Of Circular Orbits In the Majumdar-mentioning
confidence: 93%