Green's function of a massless scalar field in curved space-time and superluminal phase velocity of the retarded potential
De-Chang Dai, Dejan Stojkovic

TL;DR
This paper derives an exact solution for a massless scalar field in curved space-time, revealing that its retarded potential can have a position-dependent phase velocity exceeding the speed of light, especially near horizons.
Contribution
It provides an analytic solution showing superluminal phase velocities for a massless scalar field in curved space-time, a phenomenon previously associated mainly with massive fields.
Findings
Phase velocity of the scalar potential can surpass light speed at certain points.
Near the Schwarzschild horizon, phase velocity becomes infinitely faster than light.
Superluminal phase velocities are possible even for massless fields due to mode properties.
Abstract
We study a retarded potential solution of a massless scalar field in curved space-time. In a special ansatz for a particle at rest whose magnitude of the (scalar) charge is changing with time, we found an exact analytic solution. The solution indicates that the phase velocity of the retarded potential of a non-moving scalar charge is position dependent, and may easily be greater than the speed of light at a given point. In the case of the Schwarzschild space-time, at the horizon, the phase velocity becomes infinitely faster than the coordinate speed of light at that point. Superluminal phase velocity is relatively common phenomenon, with the the phase velocity of the massive Klein-Gordon field as the best known example. We discuss why it is possible to have modes with superluminal phase velocity even for a massless field.
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