Is the Exponential of the Chern-Simons Action a Normalizable Physical State?
arXiv:gr-qc/9402034 · doi:10.1088/0264-9381/12/2/012
Abstract
We determine the wavefunction that corresponds to the exponential of the Chern-Simons action in a family of gravitational models provided with cosmological constant whose non-perturbative canonical quantization is completely known. We show that this wavefunction does not represent a proper quantum state, because it is not normalizable with respect to the unique inner product of Lorentzian gravity.
13 pages (LATEX), Preprint CGPG-94/2-2
References in corpus (8)
- Canonical Quantization of Spherically Symmetric Gravity in Ashtekar's Self-Dual Representation
- Jones Polynomials for Intersecting Knots as Physical States of Quantum Gravity
- Minisuperspaces: Observables and Quantization
- How the Jones Polynomial Gives Rise to Physical States of Quantum General Relativity
- Unique determination of an inner product by adjointness relations in the algebra of quantum observables
- Brst Cohomology and Invariants of 4D Gravity in Ashtekar Variables
- Non-Perturbative Canonical Quantization of Minisuperspace Models: Bianchi Types I and II
- Reality Conditions in Nonperturbative Quantum Cosmology
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- Instanton representation of Plebanski gravity: XIII. Canonical structure of the Petrov classification of nondegenerate spacetimes
- Instanton representation of Plebanski gravity: XVIII. Quantization and proposed resolution of the Kodama state