Z. Stuchlik et S. Hledik, Equatorial photon motion in the Kerr-Newman spacetimes with a non-zero cosmological constant, CLASS QUANT, 17(21), 2000, pp. 4541-4576
Discussion of the equatorial photon motion in Kerr-Newman black-hole and na
ked-singularity spacetimes with a non-zero cosmological constant is present
ed. Both repulsive and attractive cosmological constants are considered. An
appropriate 'effective potential' governing the photon radial motion is de
fined, circular photon orbits are determined, and their stability with resp
ect to radial perturbations is established. The spacetimes are divided into
separated classes according to the properties of the 'effective potential'
. There is a special class of Kerr-Newman-de Sitter black-hole spacetimes w
ith the restricted repulsive barrier. In such spacetimes, photons with high
positive End all negative values of their impact parameter can travel free
ly between the outerblack-hole horizon and the cosmological horizon due to
an interplay between the rotation of the source and the cosmological repuls
ion. It is shown that this type of behaviour of the photon motion is connec
ted to an unusual relation between the values of the impact parameters of t
he photons and their directional angles relative to the outward radial dire
ction as measured in the locally non-rotating frames. Surprisingly, some ph
otons counterrotating in these frames have a positive impact parameter. Suc
h photons can be both escaping or captured in the black-hole spacetimes wit
h the restricted repulsive barrier. For the black-hole spacetimes with a st
andard, divergent repulsive barrier of the equatorial photon motion, the co
unterrotating photons with positive impact parameters must all be captured
from the region near the black-hole enter horizon as in the case of Kerr bl
ack holes, while they all escape from the region near the cosmological hori
zon. Further, the azimuthal motion is discussed and photon trajectories are
given in typical situations. It is shown that for some photons with negati
ve impact parameter turning points of their azimuthal motion can exist.