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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...

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Detalles Bibliográficos
Autores principales: Chou, C.L., Lai, H.L., Yuan, C.P.
Lenguaje:eng
Publicado: 2000
Materias:
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.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2000
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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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