Dilaton and Second-Rank Tensor Fields as Supersymmetric Compensators
| dc.creator | Nishino, Hitoshi | |
| dc.creator | Rajpoot, Subhash | |
| dc.date | 2007-12-30 | |
| dc.date.accessioned | 2026-07-07T11:54:54Z | |
| dc.date.available | 2026-07-07T11:54:54Z | |
| dc.description | We formulate a supersymmetric theory in which both a dilaton and a second-rank tensor play roles of compensators. The basic off-shell multiplets are a linear multiplet (B_{μν}, χ, ϕ) and a vector multiplet (A_μ, ł; C_{μνρ}), where ϕand B_{\m\n} are respectively a dilaton and a second-rank tensor. The third-rank tensor C_{μνρ} in the vector multiplet is 'dual' to the conventional D-field with 0 on-shell or 1 off-shell degree of freedom. The dilaton ϕis absorbed into one longitudinal component of A_μ, making it massive. Initially, B_{μν} has 1 on-shell or 3 off-shell degrees of freedom, but it is absorbed into the longitudinal components of C_{μνρ}. Eventually, C_{μνρ} with 0 on-shell or 1 off-shell degree of freedom acquires in total 1 on-shell or 4 off-shell degrees of freedom, turning into a propagating massive field. These basic multiplets are also coupled to chiral multiplets and a supersymmetric Dirac-Born-Infeld action. Some of these results are also reformulated in superspace. The proposed mechanism may well provide a solution to the long-standing puzzle of massless dilatons and second-rank tensors in supersymmetric models inspired by string theory. | |
| dc.description | 15 pages, no figures | |
| dc.identifier | https://arxiv.org/abs/0801.0106 | |
| dc.identifier | http://arxiv.org/abs/0801.0106 | |
| dc.identifier | Phys.Rev.D76:065004,2007 | |
| dc.identifier | doi:10.1103/PhysRevD.76.065004 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/205073 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Dilaton and Second-Rank Tensor Fields as Supersymmetric Compensators | |
| dc.type | text |