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Supersymmetric dark matter in the light of LEP1.5

We discuss the lower limit on the mass of the neutralino \chi that can be obtained by combining data from e^+e^- annihilation at LEP and elsewhere with astrophysical and theoretical considerations. Loopholes in the purely experimental analysis of ALEPH data from the Z peak and LEP 1.5, which appear...

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Detalles Bibliográficos
Autores principales: Ellis, John R., Falk, Toby, Olive, Keith A., Schmitt, Michael
Lenguaje:eng
Publicado: 1996
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(96)01130-6
http://cds.cern.ch/record/306954
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author Ellis, John R.
Falk, Toby
Olive, Keith A.
Schmitt, Michael
author_facet Ellis, John R.
Falk, Toby
Olive, Keith A.
Schmitt, Michael
author_sort Ellis, John R.
collection CERN
description We discuss the lower limit on the mass of the neutralino \chi that can be obtained by combining data from e^+e^- annihilation at LEP and elsewhere with astrophysical and theoretical considerations. Loopholes in the purely experimental analysis of ALEPH data from the Z peak and LEP 1.5, which appear when \mu<0 for certain values of the sneutrino mass m_{\tilde\nu} and the ratio \tan\beta of supersymmetric Higgs vacuum expectation values, may be largely or totally excluded by data from lower-energy e^+e^- data, the hypothesis that most of the cosmological dark matter consists of \chi particles, and the assumption that electroweak symmetry breaking is triggered by radiative corrections due to a heavy top quark. The combination of these inputs imposes m_{\chi} \ge 21.4~\gev, if soft supersymmetry-breaking masses are assumed to be universal at the grand-unification scale.
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publishDate 1996
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spelling cern-3069542023-03-14T18:53:47Zdoi:10.1016/0370-2693(96)01130-6http://cds.cern.ch/record/306954engEllis, John R.Falk, TobyOlive, Keith A.Schmitt, MichaelSupersymmetric dark matter in the light of LEP1.5Particle Physics - PhenomenologyWe discuss the lower limit on the mass of the neutralino \chi that can be obtained by combining data from e^+e^- annihilation at LEP and elsewhere with astrophysical and theoretical considerations. Loopholes in the purely experimental analysis of ALEPH data from the Z peak and LEP 1.5, which appear when \mu<0 for certain values of the sneutrino mass m_{\tilde\nu} and the ratio \tan\beta of supersymmetric Higgs vacuum expectation values, may be largely or totally excluded by data from lower-energy e^+e^- data, the hypothesis that most of the cosmological dark matter consists of \chi particles, and the assumption that electroweak symmetry breaking is triggered by radiative corrections due to a heavy top quark. The combination of these inputs imposes m_{\chi} \ge 21.4~\gev, if soft supersymmetry-breaking masses are assumed to be universal at the grand-unification scale.We discuss the lower limit on the mass of the neutralino $\chi$ that can be obtained by combining data from $e~+e~-$ annihilation at LEP and elsewhere with astrophysical and theoretical considerations. Loopholes in the purely experimental analysis of ALEPH data from the Z peak and LEP 1.5, which appear when $\mu<0$ for certain values of the sneutrino mass $m_{\tilde\nu}$ and the ratio $\tan\beta$ of supersymmetric Higgs vacuum expectation values, may be largely or totally excluded by data from lower-energy $e~+e~-$ data, the hypothesis that most of the cosmological dark matter consists of $\chi$ particles, and the assumption that electroweak symmetry breaking is triggered by radiative corrections due to a heavy top quark. The combination of these inputs imposes $m_{\chi} \ge 21.4\gev$, if soft supersymmetry-breaking masses are assumed to be universal at the grand-unification scale.We discuss the lower limit on the mass of the neutralino χ that can be obtained by combining data from e + e − annihilation at LEP and elsewhere with astrophysical and theoretical considerations. Loopholes in the purely experimental analysis of ALEPH data from the Z 0 peak and LEP 1.5, which appear when μ < 0 for certain values of the sneutrino mass m ν and the ratio tan β of supersymmetric Higgs vacuum expectation values, may be largely or totally excluded by data from lower-energy e + e − experiments, the hypothesis that most of the cosmological dark matter consists of χ particles, and the assumption that electroweak symmetry breaking is triggered by radiative corrections due to a heavy top quark. The combination of these inputs imposes m χ ≥ 21.4 GeV, if soft supersymmetry-breaking masses are assumed to be universal at the grand-unification scale.hep-ph/9607292CERN-TH-96-102CERN-PPE-96-84UMN-TH-1501-96TPI-MINN-96-09CERN-ALEPH-PUB-96-008CERN-PPE-96-084CERN-TH-96-102TPI-MINN-96-09UMN-TH-1501oai:cds.cern.ch:3069541996
spellingShingle Particle Physics - Phenomenology
Ellis, John R.
Falk, Toby
Olive, Keith A.
Schmitt, Michael
Supersymmetric dark matter in the light of LEP1.5
title Supersymmetric dark matter in the light of LEP1.5
title_full Supersymmetric dark matter in the light of LEP1.5
title_fullStr Supersymmetric dark matter in the light of LEP1.5
title_full_unstemmed Supersymmetric dark matter in the light of LEP1.5
title_short Supersymmetric dark matter in the light of LEP1.5
title_sort supersymmetric dark matter in the light of lep1.5
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0370-2693(96)01130-6
http://cds.cern.ch/record/306954
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AT falktoby supersymmetricdarkmatterinthelightoflep15
AT olivekeitha supersymmetricdarkmatterinthelightoflep15
AT schmittmichael supersymmetricdarkmatterinthelightoflep15