Sm. Kopeikin et al., Astrometric and timing effects of gravitational waves from localized sources - art. no. 084023, PHYS REV D, 5908(8), 1999, pp. 4023
The extremely high precision of current radio interferometric observations
demands a better theoretical treatment of secondary effects in the propagat
ion of electromagnetic signals in variable gravitational fields. Such field
s include those of oscillating and precessing stars, stationary or coalesci
ng binary systems, and colliding galaxies. Especially important is the prob
lem of propagation of light rays in the field of gravitational waves emitte
d by a localized source of gravitational radiation. A consistent approach f
or a complete and exhaustive solution of this problem is developed in the p
resent paper in the first post-Minkowskian and quadrupole approximation of
general relativity. This approximation is linear with respect to the univer
sal gravitational constant G and accounts for the static monopole, spin, an
d time-dependent quadrupole moments of an isolated system. We demonstrate f
or the first time that the equations of light propagation in the retarded g
ravitational field of an arbitrary localized source emitting quadrupole gra
vitational waves can be integrated exactly in closed form. The influence of
the gravitational field under consideration on the light propagation is ex
amined not only in the wave zone but also in cases when light passes throug
h the intermediate and near zones of the source. We reproduce the known res
ults of integration of equations of light rays, both in a stationary gravit
ational held and in the field of plane gravitational waves. establishing th
e relationship between our new formalism and the simplified approaches of o
ther authors. Explicit analytic expressions fur light deflection and integr
ated time delay Shapiro effect are obtained accounting for all possible ret
ardation effects and arbitrary relative locations of the source of gravitat
ional waves, the source of light rays, and the observer. Coordinate depende
nt terms in the expressions for observable quantities are singled out and u
sed for physically meaningful interpretation of observable quantities. It i
s shown that the ADM and harmonic gauge conditions can both be satisfied si
multaneously outside the source of gravitational waves, Such ADM-harmonic c
oordinates are extensively used in the present paper. Their use drastically
simplifies the integration of light propagation equations and the equation
s for the motion of light source and observer in the gravitational field of
the source of gravitational waves, leading to the unique interpretation of
observable effects.
The two limiting cases of small and large values of impact parameter d are
elaborated in more detail. It is proved that leading order terms for the ef
fect of light deflection in thr case of small impact parameter depend neith
er on the radiative part (similar to l/d) of the gravitational field nor on
the intermediate (similar to l/d(2)) zone terms, confirming a previous res
ult in the literature. The main effect rather comes from the near zone (sim
ilar to l/d(3)) terms. This properly of strong suppression of the influence
of gravitational waves on the propagation of light rays makes much more di
fficult any direct detection of gravitational waves by VLBI or pulsar timin
g techniques, in contrast with previous claims by other authors. We also pr
esent a thorough-going analytical treatment of time delay anti bending of l
ight in the case of large impact parameter. This exploration essentially ex
tends previous results regarding propagation of light rays in the field of
a plane monochromatic gravitational wave. Explicit expressions for Shapiro
effect and deflection angle an obtained in terms of the transverse-traceles
s (TT) part of the space-space components of the metric tensor. We also dis
cuss the relevance of the developed formalism for interpretation of radio i
nterferometric and timing observations, as well as for data processing algo
rithms for future gravitational wave detectors. [S0556-2821(99)03706-6].