Running Coupling in pure gauge theories using the Schrödinger functional
| dc.creator | Narayanan, Rajamani | |
| dc.date | 1992-11-30 | |
| dc.date.accessioned | 2026-07-07T03:39:22Z | |
| dc.date.available | 2026-07-07T03:39:22Z | |
| dc.description | Schrödinger functional, the propagation kernel for going from some field configuration at time $x^0=0$ to some other configuration at $x^0=T$, is used to define a running coupling, $\bar g^2(L)$, at a length scale, $L$, in pure gauge theories. Using a lattice formulation and finite size scaling techniques, this running coupling is calculated non-perturbatively in the continuum for a wide range of $L$, that extends from the perturbative scales to non-perturbative scales, for the specific case of pure SU(2) gauge theory. | |
| dc.description | 4 pages, RU-92-54 | |
| dc.identifier | https://arxiv.org/abs/hep-lat/9211066 | |
| dc.identifier | http://arxiv.org/abs/hep-lat/9211066 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/38897 | |
| dc.subject | High Energy Physics - Lattice | |
| dc.title | Running Coupling in pure gauge theories using the Schrödinger functional | |
| dc.type | text |