No-go theorem for gravivector and graviscalar on the brane
| dc.creator | Myung, Y. S. | |
| dc.date | 2000-10-24 | |
| dc.date | 2001-03-06 | |
| dc.date.accessioned | 2026-07-07T04:10:47Z | |
| dc.date.available | 2026-07-07T04:10:47Z | |
| dc.description | We prove the no-go theorem that the gravivector $(h_{5μ})$ and graviscalar $(h_{55})$ cannot have any on-shell propagation on the Randall-Sundrum (RS) brane. For this purpose, we analyze all of their linearized equations with the de Donder gauge (5D transverse-tracefree gauge). But we do not introduce any matter source. We use the Z$_2$-symmetry argument and their ($h_{5μ}, h_{55}$) compatibility conditions with the tensor $h_{\mn}$-equation. It turns out that $h_{55}$ does not have any bulk (massive) and brane (massless) propagations. Although $h_{5μ}$ has a sort of massive propagations, they do not belong to the physical solution. Hence we confirm that the Randall-Sundrum gauge suffices the on-shell brane physics. | |
| dc.description | 9 pages, comments and references added | |
| dc.identifier | https://arxiv.org/abs/hep-th/0010208 | |
| dc.identifier | http://arxiv.org/abs/hep-th/0010208 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/50335 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | No-go theorem for gravivector and graviscalar on the brane | |
| dc.type | text |