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Limits on Sparticle Dark Matter

Arguments are given that the lightest supersymmetric particle should be a neutralino $\chi$. Minimizing the fine tuning of the gauge hierarchy favours space of the MSSM from the stability of the electroweak vacuum. Co-annihilation with the next-to-lightest supersymmetric particle is potentially sign...

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Autor principal: Ellis, John R.
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.1063/1.59452
http://cds.cern.ch/record/380498
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author Ellis, John R.
author_facet Ellis, John R.
author_sort Ellis, John R.
collection CERN
description Arguments are given that the lightest supersymmetric particle should be a neutralino $\chi$. Minimizing the fine tuning of the gauge hierarchy favours space of the MSSM from the stability of the electroweak vacuum. Co-annihilation with the next-to-lightest supersymmetric particle is potentially significant. Incorporating the latest accelerator constraints from LEP and elsewhere, we find that 50 GeV $\lappeq m_\chi \lappeq$ 600 GeV and $\tan\beta \gappeq$ 2.5, if soft supersymmetry breaking parameters are assumed to be universal.
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institution Organización Europea para la Investigación Nuclear
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publishDate 1999
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spelling cern-3804982019-09-30T06:29:59Zdoi:10.1063/1.59452http://cds.cern.ch/record/380498engEllis, John R.Limits on Sparticle Dark MatterAstrophysics and AstronomyArguments are given that the lightest supersymmetric particle should be a neutralino $\chi$. Minimizing the fine tuning of the gauge hierarchy favours space of the MSSM from the stability of the electroweak vacuum. Co-annihilation with the next-to-lightest supersymmetric particle is potentially significant. Incorporating the latest accelerator constraints from LEP and elsewhere, we find that 50 GeV $\lappeq m_\chi \lappeq$ 600 GeV and $\tan\beta \gappeq$ 2.5, if soft supersymmetry breaking parameters are assumed to be universal.Arguments are given that the lightest supersymmetric particle should be a neutralino $\chi$. Minimizing the fine tuning of the gauge hierarchy favours $\Omega_{\chi} h^2 \sim 0.1$. There are important constraints on the parameter space of the MSSM from the stability of the electroweak vacuum. Co-annihilation with the next-to-lightest supersymmetric particle is potentially significant. Incorporating the latest accelerator constraints from LEP and elsewhere, we find that 50 GeV $\lappeq m_\chi \lappeq$ 600 GeV and $\tan\beta \gappeq$ 2.5, if soft supersymmetry breaking parameters are assumed to be universal.Arguments are given that the lightest supersymmetric particle should be a neutralino χ. Minimizing the fine tuning of the gauge hierarchy favours Ωχh2∼0.1. There are important constraints on the parameter space as the MSSM from the stability of the electroweak vacuum. Co-annihilation with the next-to-lightest supersymmetric particle is potentially significant. Incorporating the latest accelerator constraints from LEP and elsewhere, we find that 50 GeV≲mχ≲600 GeV and tan β≳2.5. if soft supersymmetry breaking parameters are assumed to be universal.astro-ph/9903003CERN-TH-99-41CERN-TH-99-041oai:cds.cern.ch:3804981999-03-02
spellingShingle Astrophysics and Astronomy
Ellis, John R.
Limits on Sparticle Dark Matter
title Limits on Sparticle Dark Matter
title_full Limits on Sparticle Dark Matter
title_fullStr Limits on Sparticle Dark Matter
title_full_unstemmed Limits on Sparticle Dark Matter
title_short Limits on Sparticle Dark Matter
title_sort limits on sparticle dark matter
topic Astrophysics and Astronomy
url https://dx.doi.org/10.1063/1.59452
http://cds.cern.ch/record/380498
work_keys_str_mv AT ellisjohnr limitsonsparticledarkmatter