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The true radiation gauge for gravity

Published 20 Jun 2010 in gr-qc, hep-th, math-ph, and math.MP | (1006.3927v3)

Abstract: Corresponding to the similarity between the Lorentz gauge $\partial_\mu A\mu=0$ in electrodynamics and $g{\mu\nu}\Gamma\rho_{\mu\nu}=0$ in gravity, we show that the counterpart of the radiation gauge $\partial_iAi=0$ is $g{ij}\Gamma\rho_{ij}=0$, in stead of other forms as discussed before. Particularly: 1) at least for a weak field, $g{ij}\Gamma\rho_{ij}=0$ fixes the gauge completely and picks out exactly the two physical components of the gravitational field; 2) like $A0$, the non-dynamical components $h_{0\mu}$ are solved instantaneously; 3) gravitational radiation is generated by the "transverse" part of the energy-momentum tensor, similar to the transverse current $\vec J_\perp$. This true" radiation gauge $g{ij}\Gamma\rho_{ij}=0$ is especially pertinent for studying gravitational energy, such as the energy flow in gravitational radiation. It agrees with the transverse-traceless (TT) gauge for a pure wave, and reveals remarkably how the TT gauge can be adapted in the presence of source.

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