We study the general motion of photons in the Kerr–de Sitter black-hole and naked singularity spacetimes. The motion is governed by the impact parameters X, related to the axial symmetry of the spacetime, and q, related to its hidden symmetry. Appropriate ‘effective potentials’ governing the latitudinal and radial motion are introduced and their behavior is examined by the ‘Chinese boxes’ technique giving regions allowed for the motion in terms of the impact parameters. Restrictions on the impact parameters X and q are established in dependence on the spacetime parameters $$M, \Lambda , a$$. The motion can be of orbital type (crossing the equatorial plane, $$q>0$$) and vortical type (tied above or below the equatorial plane, $$q<0$$). It is...
We have studied the null geodesics in the background of the Kerr–Newman black hole veiled by a plasm...
Photon region (PR) in the strong gravitational field is defined as a compact region where photons ca...
The Wyman's solution depends on two parameters, the mass M and the scalar charge σ. If one fixes M t...
Abstract We study the general motion of photons in the Kerr–de Sitter black-hole and naked singulari...
Abstract For the Kerr naked singularity (KNS) spacetimes, we study properties of spherical photon or...
© 2019 American Physical Society. Recently, several new characteristics have been introduced to desc...
Circular motion of test particles in the equatorial plane of the Kerr–Newman–de Sitter (KNdS) spacet...
We investigate in detail the circular motion of test particles in the equatorial plane of the ergore...
We briefly overview the basic properties and generic behavior of circular equatorial particle orbits...
Abstract We construct the light escape cones of isotropic spot sources of radiation residing in spec...
We analyze the properties of circular orbits of test particles on the equatorial plane of a rotating...
International audienceWe consider a class of static and spherically symmetric black hole geometries ...
In this paper, we investigate the light trajectories and shadow properties in the rotating version o...
The timelike and null geodesics in the Kerr metric describe important properties of the space surrou...
We provide a complete characterization of the metric Killing bundles (or metric bundles) of the Kerr...
We have studied the null geodesics in the background of the Kerr–Newman black hole veiled by a plasm...
Photon region (PR) in the strong gravitational field is defined as a compact region where photons ca...
The Wyman's solution depends on two parameters, the mass M and the scalar charge σ. If one fixes M t...
Abstract We study the general motion of photons in the Kerr–de Sitter black-hole and naked singulari...
Abstract For the Kerr naked singularity (KNS) spacetimes, we study properties of spherical photon or...
© 2019 American Physical Society. Recently, several new characteristics have been introduced to desc...
Circular motion of test particles in the equatorial plane of the Kerr–Newman–de Sitter (KNdS) spacet...
We investigate in detail the circular motion of test particles in the equatorial plane of the ergore...
We briefly overview the basic properties and generic behavior of circular equatorial particle orbits...
Abstract We construct the light escape cones of isotropic spot sources of radiation residing in spec...
We analyze the properties of circular orbits of test particles on the equatorial plane of a rotating...
International audienceWe consider a class of static and spherically symmetric black hole geometries ...
In this paper, we investigate the light trajectories and shadow properties in the rotating version o...
The timelike and null geodesics in the Kerr metric describe important properties of the space surrou...
We provide a complete characterization of the metric Killing bundles (or metric bundles) of the Kerr...
We have studied the null geodesics in the background of the Kerr–Newman black hole veiled by a plasm...
Photon region (PR) in the strong gravitational field is defined as a compact region where photons ca...
The Wyman's solution depends on two parameters, the mass M and the scalar charge σ. If one fixes M t...