Hamiltonian formalism and gauge-fixing conditions for cosmological perturbation theory
arXiv:1810.11621 · doi:10.1088/1361-6382/ab45aa
Abstract
We apply the Dirac procedure for constrained systems to the Arnowitt-Deser-Misner formalism linearized around the Friedmann-Lemaitre universe. We explain and employ some basic concepts such as Dirac observables, Dirac brackets, gauge-fixing conditions, reduced phase space, physical Hamiltonian and physical dynamics. In particular, we elaborate on the key concept which is the canonical isomorphism between different gauge-fixing surfaces. We apply our formalism to describe the reduced phase space of cosmological perturbations in some popular in the literature gauges. Our formalism is first developed for the universe with a single fluid and then extended to the multi-fluid case. The obtained results are a starting point for complete quantization of the cosmological perturbations and the cosmological background. Our approach may be used in future to derive the reduced phase space of higher order perturbations and in more generic cosmological spacetimes.
38 pages, 1 figure, includes a discussion of the relation between the Dirac observables and the gauge-invariant variables such as the Bardeen potentials or the Mukhanov-Sasaki variable
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Cited by in corpus (7)
- Unitarity of quantum-gravitational corrections to primordial fluctuations in the Born-Oppenheimer approach
- Observations in Quantum Cosmology
- Ambiguous power spectrum from a quantum bounce
- Quantum entanglement and non-Gaussianity in the primordial Universe
- Gauge-fixing and spacetime reconstruction in the Hamiltonian theory of cosmological perturbations
- Dirac procedure and the Hamiltonian formalism for cosmological perturbations in a Bianchi I universe
- Unitarily inequivalent quantum cosmological bouncing models