Geometry of N=4, d=1 nonlinear supermultiplet
| dc.creator | Bellucci, S. | |
| dc.creator | Krivonos, S. | |
| dc.date | 2006-11-09 | |
| dc.date.accessioned | 2026-07-07T11:23:03Z | |
| dc.date.available | 2026-07-07T11:23:03Z | |
| dc.description | We construct the general action for $N=4, d=1$ nonlinear supermultiplet including the most general interaction terms which depend on the arbitrary function $h$ obeying the Laplace equation on $S^3$. We find the bosonic field $B$ which depends on the components of nonlinear supermultiplet and transforms as a full time derivative under N=4 supersymmetry. The most general interaction is generated just by a Fayet-Iliopoulos term built from this auxiliary component. Being transformed through a full time derivative under $N=4, d=1$ supersymmetry, this auxiliary component $B$ may be dualized into a fourth scalar field giving rise to a four dimensional $N=4, d=1$ sigma-model. We analyzed the geometry in the bosonic sector and find that it is not a hyper-Kähler one. With a particular choice of the target space metric $g$ the geometry in the bosonic sector coincides with the one which appears in heterotic $(4,0)$ sigma-model in $d=2$. | |
| dc.description | 9 pages, LaTeX file, PACS: 11.30.Pb, 03.65.-w | |
| dc.identifier | https://arxiv.org/abs/hep-th/0611104 | |
| dc.identifier | http://arxiv.org/abs/hep-th/0611104 | |
| dc.identifier | Phys.Rev.D74:125024,2006 | |
| dc.identifier | doi:10.1103/PhysRevD.74.125024 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/194773 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Geometry of N=4, d=1 nonlinear supermultiplet | |
| dc.type | text |