Compatibility of radial, Lorenz and harmonic gauges
arXiv:0704.0992 · doi:10.1103/PhysRevD.76.084013
Abstract
We observe that the radial gauge can be consistently imposed \emph{together} with the Lorenz gauge in Maxwell theory, and with the harmonic traceless gauge in linearized general relativity. This simple observation has relevance for some recent developments in quantum gravity where the radial gauge is implicitly utilized.
9 pages, minor changes in the bibliography
References in corpus (14)
- Background Independent Quantum Gravity: A Status Report
- Discreteness of area and volume in quantum gravity
- General relativity as an effective field theory: The leading quantum corrections
- Quantum Theory of Gravity I: Area Operators
- Weaving a classical geometry with quantum threads
- Graviton propagator from background-independent quantum gravity
- Particle scattering in loop quantum gravity
- Group Integral Techniques for the Spinfoam Graviton Propagator
- Towards the graviton from spinfoams: higher order corrections in the 3d toy model
- Towards the graviton from spinfoams: the 3d toy model
- A Review of Leading Quantum Gravitational Corrections to Newtonian Gravity
- Radial propagators and Wilson loops
- The radial gauge propagators in quantum gravity
- Feynman rules in radial gauge
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