Phys. Rev. D 40, 1048–1052 (1989)Unimodular theory of canonical quantum gravityReceived 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:
|
