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New Production Mechanism of Neutral Higgs Bosons with Right scalar tau neutrino as the LSP
Motived by the neutrino oscillation data, we consider the lightest tau sneutrino $\tilde \nu_{\tau_1}$ (which is mostly the right tau sneutrino) to be the lightest supersymmetric particle (LSP) in the framework of the minimal supersymmetric Standard Model with see-saw mechanism. Both the standard an...
Autores principales: | , , |
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Lenguaje: | eng |
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2000
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Acceso en línea: | https://dx.doi.org/10.1016/S0370-2693(00)00933-3 http://cds.cern.ch/record/445297 |
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author | Chou, C.L. Lai, H.L. Yuan, C.P. |
author_facet | Chou, C.L. Lai, H.L. Yuan, C.P. |
author_sort | Chou, C.L. |
collection | CERN |
description | Motived by the neutrino oscillation data, we consider the lightest tau sneutrino $\tilde \nu_{\tau_1}$ (which is mostly the right tau sneutrino) to be the lightest supersymmetric particle (LSP) in the framework of the minimal supersymmetric Standard Model with see-saw mechanism. Both the standard and the non-standard trilinear scalar coupling terms are included for the right tau sneutrino interactions. The decay branching ratio of $\tilde \nu_{\tau_2} \to \tilde \nu_{\tau_1}+ h^0$ can become so large that the production rate of the lightest neutral Higgs boson ($h^0$) can be largely enhanced at electron or hadron colliders, either from the direct production of $\tilde \nu_{\tau_2}$ or from the decay of charginos, neutralinos, sleptons, and the cascade decay of squarks and gluinos, etc. Furthermore, because of the small LSP annihilation rate, $\tilde \nu_{\tau_1}$ can be a good candidate for cold dark matter. |
id | cern-445297 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2000 |
record_format | invenio |
spelling | cern-4452972023-03-14T17:09:19Zdoi:10.1016/S0370-2693(00)00933-3http://cds.cern.ch/record/445297engChou, C.L.Lai, H.L.Yuan, C.P.New Production Mechanism of Neutral Higgs Bosons with Right scalar tau neutrino as the LSPParticle Physics - PhenomenologyMotived by the neutrino oscillation data, we consider the lightest tau sneutrino $\tilde \nu_{\tau_1}$ (which is mostly the right tau sneutrino) to be the lightest supersymmetric particle (LSP) in the framework of the minimal supersymmetric Standard Model with see-saw mechanism. Both the standard and the non-standard trilinear scalar coupling terms are included for the right tau sneutrino interactions. The decay branching ratio of $\tilde \nu_{\tau_2} \to \tilde \nu_{\tau_1}+ h^0$ can become so large that the production rate of the lightest neutral Higgs boson ($h^0$) can be largely enhanced at electron or hadron colliders, either from the direct production of $\tilde \nu_{\tau_2}$ or from the decay of charginos, neutralinos, sleptons, and the cascade decay of squarks and gluinos, etc. Furthermore, because of the small LSP annihilation rate, $\tilde \nu_{\tau_1}$ can be a good candidate for cold dark matter.Motived by the neutrino oscillation data, we consider the lightest tau sneutrino $\tilde \nu_{\tau_1}$ (which is mostly the right tau sneutrino) to be the lightest supersymmetric particle (LSP) in the framework of the minimal supersymmetric Standard Model. Both the standard and the non-standard trilinear scalar coupling terms are included for the right tau sneutrino interactions. The decay branching ratio of $\tilde \nu_{\tau_2} \to \tilde \nu_{\tau_1}+ h^0$ can become so large that the production rate of the lightest neutral Higgs boson ($h^0$) can be largely enhanced at electron or hadron colliders, either from the direct production of $\tilde \nu_{\tau_2}$ or from the decay of charginos, neutralinos, sleptons, and the cascade decay of squarks and gluinos, etc. Furthermore, because of the small LSP annihilation rate, $\tilde \nu_{\tau_1}$ can be a good candidate for cold dark matter.Inspired by the neutrino oscillation data, we consider the lightest tau sneutrino ν ̃ τ 1 (which is mostly the right tau sneutrino) to be the lightest supersymmetric particle (LSP) in the framework of the minimal supersymmetric Standard Model. Both the standard and the non-standard trilinear scalar coupling terms are included for the right tau sneutrino interactions. The decay branching ratio of ν ̃ τ 2 → ν ̃ τ 1 +h 0 can become so large that the production rate of the lightest neutral Higgs boson ( h 0 ) can be largely enhanced at electron or hadron colliders, either from the direct production of ν ̃ τ 2 or from the decay of charginos, neutralinos, sleptons, and the cascade decay of squarks and gluinos, etc. Furthermore, because of the small LSP annihilation rate, ν ̃ τ 1 can be a good candidate for cold dark matter.hep-ph/0006313CERN-TH-2000-182CERN-TH-2000-182oai:cds.cern.ch:4452972000-06-28 |
spellingShingle | Particle Physics - Phenomenology Chou, C.L. Lai, H.L. Yuan, C.P. New Production Mechanism of Neutral Higgs Bosons with Right scalar tau neutrino as the LSP |
title | New Production Mechanism of Neutral Higgs Bosons with Right scalar tau neutrino as the LSP |
title_full | New Production Mechanism of Neutral Higgs Bosons with Right scalar tau neutrino as the LSP |
title_fullStr | New Production Mechanism of Neutral Higgs Bosons with Right scalar tau neutrino as the LSP |
title_full_unstemmed | New Production Mechanism of Neutral Higgs Bosons with Right scalar tau neutrino as the LSP |
title_short | New Production Mechanism of Neutral Higgs Bosons with Right scalar tau neutrino as the LSP |
title_sort | new production mechanism of neutral higgs bosons with right scalar tau neutrino as the lsp |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/S0370-2693(00)00933-3 http://cds.cern.ch/record/445297 |
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