Double beta decay in left-right symmetric models
| dc.creator | Hirsch, M. | |
| dc.creator | Klapdor-Kleingrothaus, H. V. | |
| dc.creator | Panella, O. | |
| dc.date | 1996-02-14 | |
| dc.date.accessioned | 2026-07-07T11:35:13Z | |
| dc.date.available | 2026-07-07T11:35:13Z | |
| dc.description | Left-right symmetric models provide a natural framework for neutrinoless double beta ($\znbb$) decay. In the analysis of $\znbb$ decay in left-right symmetric models, however, it is usually assumed that all neutrinos are light. On the other hand, heavy {\it right-handed} neutrinos appear quite naturally in left-right symmetric models and should therefore not be neglected. Assuming the existence of at least one right-handed heavy neutrino, absence of $\znbb$ decay of $^{76}$Ge currently provides the following limits on the mass and mixing angle of right-handed W-bosons: $m_{W_R}\ge 1.1 $ TeV and $\tan(ζ) \le 4.7 \times 10^{-3}$ for a particular value of the effective right-handed neutrino mass, $\emnv = 1$ TeV, and in the limit of infinitly massive doubly charged Higgs ($Δ^{--}$). The effects of the inclusion of the Higgs triplet on $\znbb$ decay are also discussed. | |
| dc.description | LaTeX, 9 pages, 3 figures | |
| dc.identifier | https://arxiv.org/abs/hep-ph/9602306 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/9602306 | |
| dc.identifier | Phys.Lett.B374:7-12,1996 | |
| dc.identifier | doi:10.1016/0370-2693(96)00185-2 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/198518 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Double beta decay in left-right symmetric models | |
| dc.type | text |