Limitations of the adiabatic approximation to the gravitational self-force

Abstract

A small body moving in the field of a much larger black hole and subjected to its own gravity moves on an accelerated world line in the background spacetime of the large black hole. The acceleration is produced by the body's gravitational self-force, which is constructed from the body's retarded gravitational field. The adiabatic approximation to the gravitational self-force is obtained instead from the half-retarded minus half-advanced field. It is much easier to compute, and it is known to produce the same dissipative effects as the true self-force. We argue that the adiabatic approximation is limited, because it discards important conservative terms which lead to the secular evolution of some orbital elements. We argue further that this secular evolution has measurable consequences; in particular, it affects the phasing of the orbit and the phasing of the associated gravitational wave. Our argument rests on a simple toy model involving a point electric charge moving slowly in the weak gravitational field of a central mass; the charge is also subjected to its electromagnetic self-force. In this simple context the true self-force is known explicitly and it can cleanly be separated into conservative and radiation-reaction pieces. Its long-term effect on the particle's orbital elements can be fully determined. In this model we observe that the conservative part of the self-force produces a secular regression of the orbit's periapsis. We explain how the conclusions reached on the basis of the toy model can be extended to the gravitational self-force, and we attempt to extend them also to the case of rapid motions and strong fields. While the limitations of the adiabatic approximation are quite severe in a post-Newtonian context in which the motion is slow and the gravitational field weak, they may be less severe for rapid motions and strong fields.

Resonantly enhanced and diminished strong-field gravitational-wave fluxes

“…[18]. 8 One might be concerned about gauge ambiguities associated with the gravitational self force. As shown by Mino [11], these ambiguities disappear when one averages the self force's effects over an infinite time.…”

“…It makes the largest contribution to an orbit's phase evolution. The conservative piece makes a smaller (though still significant) contribution which accumulates secularly over many orbits [8,9].…”

Gravitational self-force on a particle in eccentric orbit around a Schwarzschild black hole

“…SF corrections to the precession rate have been analyzed for weak-field orbits and within the toy model of the EM SF [36,37], but never before for the gravitational problem in strong field. Our code generates the SF data necessary to tackle this problem for the first time.…”

Finding fields and self-force in a gauge appropriate to separable wave equations

“…To first order, the particle feels a self-force, whose dissipative part is the radiation-reaction force that drives the inspiral. The self-force also has a conservative part that alters the phase of the orbit and of the emitted radiation [1,2].…”