Search for Z′ bosons decaying to pairs of heavy Majorana neutrinos in proton-proton collisions at √s = 13 TeV
A search for the production of pairs of heavy Majorana neutrinos (Nℓ ) from the decays of Z′ bosons is performed using the CMS detector at the LHC. The data were collected in proton-proton collisions at a center-of-mass energy of √s = 13 TeV, with an integrated luminosity of 138 fb−1 . The signature...
| Autores: | , , , |
|---|---|
| Tipo de recurso: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2023 |
| País: | Brasil |
| Institución: | Universidade Federal do Rio Grande do Sul (UFRGS) |
| Repositorio: | Repositório Institucional da UFRGS |
| Idioma: | inglés |
| OAI Identifier: | oai:www.lume.ufrgs.br:10183/278389 |
| Acceso en línea: | http://hdl.handle.net/10183/278389 |
| Access Level: | acceso abierto |
| Palabra clave: | Aceleradores de partículas Bosons Z Colisões proton-proton Beyond standard model Hadron-Hadron scattering |
| Sumario: | A search for the production of pairs of heavy Majorana neutrinos (Nℓ ) from the decays of Z′ bosons is performed using the CMS detector at the LHC. The data were collected in proton-proton collisions at a center-of-mass energy of √s = 13 TeV, with an integrated luminosity of 138 fb−1 . The signature for the search is an excess in the invariant mass distribution of the fnal-state objects, two same-favor leptons (e or µ) and at least two jets. No signifcant excess of events beyond the expected background is observed. Upper limits at 95% confdence level are set on the product of the Z′ production cross section and its branching fraction to a pair of Nℓ , as functions of Nℓ and Z′ boson masses (mNℓ and mZ′, respectively) for mZ′ from 0.4 to 4.6 TeV and mNℓ from 0.1 TeV to mZ′/2. In the theoretical framework of a left-right symmetric model, exclusion bounds in the mNℓ -mZ′ plane are presented in both the electron and muon channels. The observed upper limit on mZ′ reaches up to 4.42 TeV. These are the most restrictive limits to date on the mass of Nℓ as a function of the Z′ boson mass. |
|---|