The reduced phase space of spherically symmetric Einstein-Maxwell theory including a cosmological constant
arXiv:gr-qc/9910007 · doi:10.1016/0550-3213(94)00564-U
Abstract
We extend here the canonical treatment of spherically symmetric (quantum) gravity to the most simple matter coupling, namely spherically symmetric Maxwell theory with or without a cosmological constant. The quantization is based on the reduced phase space which is coordinatized by the mass and the electric charge as well as their canonically conjugate momenta, whose geometrical interpretation is explored. The dimension of the reduced phase space depends on the topology chosen, quite similar to the case of pure (2+1) gravity. We investigate several conceptual and technical details that might be of interest for full (3+1) gravity. We use the new canonical variables introduced by Ashtekar, which simplifies the analysis tremendously.
37p, LATEX
Cited by in corpus (7)
- The Area Operator in the Spherically Symmetric Sector of Loop Quantum Gravity
- Quantum Symmetry Reduction for Diffeomorphism Invariant Theories of Connections
- Ricci flat rotating black branes with a conformally invariant Maxwell source
- Quantum-mechanical model of the Kerr-Newman black hole
- Spherically symmetric Einstein-Maxwell theory and loop quantum gravity corrections
- Abelian BF-Theory and Spherically Symmetric Electromagnetism
- Black holes and Rindler superspace: classical singularity and quantum unitarity