Generalized Coordinate Gauge and Nonabelian Stokes Theorem
| dc.creator | Shevchenko, V. I. | |
| dc.creator | Simonov, Yu. A. | |
| dc.date | 1998-02-19 | |
| dc.date | 1998-03-16 | |
| dc.date.accessioned | 2026-07-07T04:24:17Z | |
| dc.date.available | 2026-07-07T04:24:17Z | |
| dc.description | A contour gauge of general type is analysed where 1-form (vector potential) is expressed as a contour integral of the 2-form (field strength) along an arbitrary contour $C$. For a special class of contours the gauge condition reduces to $k_μ(x) A_μ(x) = 0 $ where $k_μ(x)$ is a tangent vector to the contour $C$. A simple proof of the nonabelian Stokes theorem is given demonstrating the advantage of the gauge. | |
| dc.description | LaTeX, revised version, comments added | |
| dc.identifier | https://arxiv.org/abs/hep-th/9802134 | |
| dc.identifier | http://arxiv.org/abs/hep-th/9802134 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/55352 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Generalized Coordinate Gauge and Nonabelian Stokes Theorem | |
| dc.type | text |