Applications of a new proposal for solving the ‘‘problem of time’’ to some simple quantum cosmological models

Atsushi Higuchi and Robert M. Wald
Phys. Rev. D 51, 544 – Published 15 January 1995
PDFExport Citation

Abstract

We apply a recent proposal for defining states and observables in quantum gravity to some simple models. First, we consider the toy model of a Klein-Gordon particle in an external potential in Minkowski spacetime and compare our proposal to the theory obtained by deparametrizing with respect to a choice of time slicing prior to quantization. We show explicitly that the dynamics defined by the deparametrization approach depends upon the choice of time slicing. On the other hand, our proposal automatically yields a well defined dynamics, manifestly independent of the choice of time slicing at intermediate times, but there is a ‘‘memory effect’’: After the potential is turned off, the dynamics no longer returns to the standard, free particle dynamics. Next, we apply our proposal to the closed Robertson-Walker quantum cosmology with a homogeneous massless scalar field. We choose our time variable to the size of the Universe, so the only dynamical variable is the scalar field. It is shown that the resulting theory has the expected semiclassical behavior up to the classical turning point from expansion to contraction; i.e., given a classical solution which expands for much longer than the Planck time, there is a quantum state whose dynamical evolution closely approximates this classical solution during the expanding phase. However, when the ‘‘time’’ takes a value larger than the classical maximum, the scalar field becomes ‘‘frozen’’ at the value it had when it entered the classically forbidden region. The Taub model, with and without a homogeneous scalar field, also is studied, and similar behavior is found. In an Appendix, we derive the form of the Wheeler-DeWitt equation on minisuperspace for the Bianchi models by performing a proper quantum reduction of the momentum constraints; this equation differs from the usual form of the Wheeler-DeWitt equation, which is obtained by solving the momentum constraints classically, prior to quantization.

  • Received 26 July 1994

DOI:https://doi.org/10.1103/PhysRevD.51.544

©1995 American Physical Society

Authors & Affiliations

Atsushi Higuchi

  • Institut für Theoretische Physik, Universität Bern, Sidlerstrasse 5, CH-3012 Bern, Switzerland

Robert M. Wald

  • Enrico Fermi Institute and Department of Physics, University of Chicago, 5640 S. Ellis Ave., Chicago, Illinois 60637-1433

References (Subscription Required)

Click to Expand
Issue

Vol. 51, Iss. 2 — 15 January 1995

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×
×

Images

×

Sign up to receive regular email alerts from Physical Review D

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×