A low upper mass limit for the central black hole in the late-type galaxy NGC 4414
(2016)
Simplified derivation of the gravitational wave stress tensor from the linearized Einstein field equations.
Proceedings of the National Academy of Sciences National Academy of Sciences (2016)
Abstract:
A conserved stress energy tensorfor weak field gravitational waves propagating in vacuum is derived directly from the linearized general relativistic wave equation alone, for an arbitrary gauge. In any harmonic gauge, the form of the tensor leads directly to the classical expression for the outgoing wave energy. The method described here, however, is a much simpler,shorter, and more physically motivated approach than is the customary procedure, which involves a lengthy and cumbersome second-order (in wave-amplitude) calculation starting with the Einstein tensor. Our method has the added advantage of exhibiting the direct coupling between the outgoing wave energy flux and the work done by the gravitational field on the sources. For nonharmonic gauges, the directly derived wave stress tensor has an apparent index asymmetry. This coordinate artifact may be straightforwardly removed, and the symmetrized (still gauge-invariant) tensor then takes on its widely used form. Angular momentum conservation follows immediately. For any harmonic gauge, however, the stress tensor found is manifestly symmetric from the start, and its derivation depends, in its entirety, on the structure of the linearized wave equation.The influence of mergers and ram-pressure stripping on black hole–bulge correlations
Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 461:4 (2016) 3533-3541
On the energy dissipation rate at the inner edge of circumbinary discs
(2016)
On the formation of planetary systems in photoevaporating transition discs
Monthly Notices of the Royal Astronomical Society Oxford University Press 464:1 (2016)