The Nature of Cosmic Time
| dc.creator | Salopek, D. S. | |
| dc.date | 1995-08-23 | |
| dc.date.accessioned | 2026-07-07T02:20:01Z | |
| dc.date.available | 2026-07-07T02:20:01Z | |
| dc.description | Hamilton-Jacobi theory provides a natural starting point for a covariant description of the gravitational field. Using a spatial gradient expansion, one may solve for the phase of the wavefunction by using a line-integral in superspace. Each contour of integration corresponds to a particular choice of time-hypersurface, and each yields the same answer. In this way, one can describe all time choices simultaneously. In an interesting application to cosmology, I compute large-angle microwave background anisotropies and the galaxy-galaxy correlation function associated with the scalar and tensor fluctuations of power-law inflation. | |
| dc.description | 8 pages, Latex 2.09, Fields Institute Publication: `Sixth Canadian Conference on General Relativity and Relativistic Astrophysics' Fredericton, Canada, May 25-27, 1995 One figure included in file | |
| dc.identifier | https://arxiv.org/abs/astro-ph/9508101 | |
| dc.identifier | http://arxiv.org/abs/astro-ph/9508101 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/10091 | |
| dc.subject | Astrophysics | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.title | The Nature of Cosmic Time | |
| dc.type | text |