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Phys. Rev. D 40, 1048–1052 (1989)

Unimodular theory of canonical quantum gravity

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W. G. Unruh
Cosmology Program, Canadian Institute for Advanced Research, and Department of Physics, University of British Columbia, Vancouver, British Columbia, Canada V6T 2A6 and Institute for Theoretical Physics, University of California, Santa Barbara, Santa Barbara, California 93106

Received 4 November 1988; published in the issue dated 15 August 1989

Einstein's theory of gravity is reformulated so that the cosmological constant becomes an integration constant of the theory, rather than a "coupling" constant. However, in the Hamiltonian form of the theory, the Hamiltonian constraint is missing, while the usual momentum constraints are still present. Replacing the Hamiltonian constraint is a secondary constraint, which introduces the cosmological constant. The quantum version has a normal "Schrödinger" form of time development, and the wave function does not obey the usual "Wheeler-DeWitt" equation, making the interpretation of the theory much simpler. The small value of the cosmological constant in the Universe at present becomes a genuine question of initial conditions, rather than a question of why one of the coupling constants has a particular value. The key "weakness" of this formulation is that one must introduce a nondynamic background spacetime volume element.

© 1989 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.40.1048
DOI:
10.1103/PhysRevD.40.1048
PACS: