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Dark Matter before the LHC in a Natural Supersymmetric Standard Model

We show that the solid lower bound of about 10^{-44} cm^2 is obtained for the cross section between the supersymmetric dark matter and nucleon in a theory in which the supersymmetric fine-tuning problem is solved without extending the Higgs sector at the weak scale. This bound arises because of rela...

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Detalles Bibliográficos
Autores principales: Kitano, R, Nomura, Y
Lenguaje:eng
Publicado: 2005
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2005.10.069
http://cds.cern.ch/record/885813
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author Kitano, R
Nomura, Y
author_facet Kitano, R
Nomura, Y
author_sort Kitano, R
collection CERN
description We show that the solid lower bound of about 10^{-44} cm^2 is obtained for the cross section between the supersymmetric dark matter and nucleon in a theory in which the supersymmetric fine-tuning problem is solved without extending the Higgs sector at the weak scale. This bound arises because of relatively small superparticle masses and a fortunate correlation that the two dominant diagrams for the dark matter detection always interfere constructively if the constraint from the b -> s \gamma measurements is obeyed. It is, therefore, quite promising in the present scenario that the supersymmetric dark matter is discovered before the LHC, assuming that the dark matter is the lightest supersymmetric particle.
id cern-885813
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2005
record_format invenio
spelling cern-8858132019-09-30T06:29:59Zdoi:10.1016/j.physletb.2005.10.069http://cds.cern.ch/record/885813engKitano, RNomura, YDark Matter before the LHC in a Natural Supersymmetric Standard ModelParticle Physics - PhenomenologyWe show that the solid lower bound of about 10^{-44} cm^2 is obtained for the cross section between the supersymmetric dark matter and nucleon in a theory in which the supersymmetric fine-tuning problem is solved without extending the Higgs sector at the weak scale. This bound arises because of relatively small superparticle masses and a fortunate correlation that the two dominant diagrams for the dark matter detection always interfere constructively if the constraint from the b -> s \gamma measurements is obeyed. It is, therefore, quite promising in the present scenario that the supersymmetric dark matter is discovered before the LHC, assuming that the dark matter is the lightest supersymmetric particle.hep-ph/0509221LBNL-58876SLAC-PUB-11487UCB-PTH-2005-29oai:cds.cern.ch:8858132005-09-21
spellingShingle Particle Physics - Phenomenology
Kitano, R
Nomura, Y
Dark Matter before the LHC in a Natural Supersymmetric Standard Model
title Dark Matter before the LHC in a Natural Supersymmetric Standard Model
title_full Dark Matter before the LHC in a Natural Supersymmetric Standard Model
title_fullStr Dark Matter before the LHC in a Natural Supersymmetric Standard Model
title_full_unstemmed Dark Matter before the LHC in a Natural Supersymmetric Standard Model
title_short Dark Matter before the LHC in a Natural Supersymmetric Standard Model
title_sort dark matter before the lhc in a natural supersymmetric standard model
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.physletb.2005.10.069
http://cds.cern.ch/record/885813
work_keys_str_mv AT kitanor darkmatterbeforethelhcinanaturalsupersymmetricstandardmodel
AT nomuray darkmatterbeforethelhcinanaturalsupersymmetricstandardmodel