A Rigorous Derivation of Gravitational Self-force
Samuel E. Gralla, Robert M. Wald

TL;DR
This paper rigorously derives the gravitational self-force equations in general relativity by analyzing a family of scaled metrics, establishing the worldline as a geodesic and identifying self-force effects as first-order perturbations.
Contribution
It provides a systematic, assumption-free derivation of the MiSaTaQuWa equations using a one-parameter family of metrics, clarifying the foundations of gravitational self-force theory.
Findings
Proves the worldline is a background geodesic in the limit.
Identifies self-force as a first-order correction in the scaling parameter.
Clarifies the status and derivation of the MiSaTaQuWa equations.
Abstract
There is general agreement that the MiSaTaQuWa equations should describe the motion of a "small body" in general relativity, taking into account the leading order self-force effects. However, previous derivations of these equations have made a number of ad hoc assumptions and/or contain a number of unsatisfactory features. For example, all previous derivations have invoked, without proper justification, the step of "Lorenz gauge relaxation", wherein the linearized Einstein equation is written down in the form appropriate to the Lorenz gauge, but the Lorenz gauge condition is then not imposed--thereby making the resulting equations for the metric perturbation inequivalent to the linearized Einstein equations. In this paper, we analyze the issue of "particle motion" in general relativity in a systematic and rigorous way by considering a one-parameter family of metrics, ,…
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