Master equation in the general gauge: on the problem of infinite reducibility
| dc.creator | Vilkovisky, G. A. | |
| dc.date | 1999-01-31 | |
| dc.date.accessioned | 2026-07-07T06:33:52Z | |
| dc.date.available | 2026-07-07T06:33:52Z | |
| dc.description | The master equation is quantized. This is an example of quantization of a gauge theory with nilpotent generators. No ghosts are needed for a generation of the gauge algebra. The point about the nilpotent generators is that one can't write down a single functional integral for this theory. One has to write down a product of two coupled functional integrals and take a square root. In the special gauge where the gauge conditions are commuting, the functional integrals decouple, and one recovers the known result. | |
| dc.description | 9 pages, no figures. Latex 2.09 | |
| dc.identifier | https://arxiv.org/abs/hep-th/9902009 | |
| dc.identifier | http://arxiv.org/abs/hep-th/9902009 | |
| dc.identifier | Lett.Math.Phys. 49 (1999) 123-130 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/99339 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Master equation in the general gauge: on the problem of infinite reducibility | |
| dc.type | text |