Zero-curvature representation for harmonic-superspace equations of motion in $N=1, D=6$ supersymmetric gauge theory
| dc.creator | Zupnik, B. M. | |
| dc.date | 1995-12-06 | |
| dc.date.accessioned | 2026-07-07T04:21:43Z | |
| dc.date.available | 2026-07-07T04:21:43Z | |
| dc.description | We consider the $SYM^1_6$ harmonic-superspace system of equations that contains superfield constraints and equations of motion for the simplest six-dimensional supersymmetric gauge theory. A special $A$-frame of the analytic basis is introduced where a kinematic equation for the harmonic connection $A^{\s--}$ can be solved . A dynamical equation in this frame is equivalent to the zero-curvature equation corresponding to the covariant conservation of analyticity. Using a simple harmonic gauge condition for the gauge group $SU(2)$ we derive the superfield equations that produce the general $SYM^1_6$ solution . An analogous approach for the analysis of integrability conditions for the $SYM^2_4$-theory and $SYM$-supergravity-matter systems in harmonic superspace is discussed briefly. | |
| dc.description | Latex file, 17 pages | |
| dc.identifier | https://arxiv.org/abs/hep-th/9512035 | |
| dc.identifier | http://arxiv.org/abs/hep-th/9512035 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/54433 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Zero-curvature representation for harmonic-superspace equations of motion in $N=1, D=6$ supersymmetric gauge theory | |
| dc.type | text |