Cargando…

Supersymmetric Dark Matter after LHC Run 1

Different mechanisms operate in various regions of the MSSM parameter space to bring the relic density of the lightest neutralino, neutralino_1, assumed here to be the LSP and thus the Dark Matter (DM) particle, into the range allowed by astrophysics and cosmology. These mechanisms include coannihil...

Descripción completa

Detalles Bibliográficos
Autores principales: Bagnaschi, E.A., Buchmueller, O., Cavanaugh, R., Citron, M., De Roeck, A., Dolan, M.J., Ellis, J.R., Flächer, H., Heinemeyer, S., Isidori, G., Malik, S., Martínez Santos, D., Olive, K.A., Sakurai, K., de Vries, K.J., Weiglein, G.
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1140/epjc/s10052-015-3718-9
http://cds.cern.ch/record/2040986
_version_ 1780947788449710080
author Bagnaschi, E.A.
Buchmueller, O.
Cavanaugh, R.
Citron, M.
De Roeck, A.
Dolan, M.J.
Ellis, J.R.
Flächer, H.
Heinemeyer, S.
Isidori, G.
Malik, S.
Martínez Santos, D.
Olive, K.A.
Sakurai, K.
de Vries, K.J.
Weiglein, G.
author_facet Bagnaschi, E.A.
Buchmueller, O.
Cavanaugh, R.
Citron, M.
De Roeck, A.
Dolan, M.J.
Ellis, J.R.
Flächer, H.
Heinemeyer, S.
Isidori, G.
Malik, S.
Martínez Santos, D.
Olive, K.A.
Sakurai, K.
de Vries, K.J.
Weiglein, G.
author_sort Bagnaschi, E.A.
collection CERN
description Different mechanisms operate in various regions of the MSSM parameter space to bring the relic density of the lightest neutralino, neutralino_1, assumed here to be the LSP and thus the Dark Matter (DM) particle, into the range allowed by astrophysics and cosmology. These mechanisms include coannihilation with some nearly-degenerate next-to-lightest supersymmetric particle (NLSP) such as the lighter stau (stau_1), stop (stop_1) or chargino (chargino_1), resonant annihilation via direct-channel heavy Higgs bosons H/A, the light Higgs boson h or the Z boson, and enhanced annihilation via a larger Higgsino component of the LSP in the focus-point region. These mechanisms typically select lower-dimensional subspaces in MSSM scenarios such as the CMSSM, NUHM1, NUHM2 and pMSSM10. We analyze how future LHC and direct DM searches can complement each other in the exploration of the different DM mechanisms within these scenarios. We find that the stau_1 coannihilation regions of the CMSSM, NUHM1, NUHM2 can largely be explored at the LHC via searches for missing E_T events and long-lived charged particles, whereas their H/A funnel, focus-point and chargino_1 coannihilation regions can largely be explored by the LZ and Darwin DM direct detection experiments. We find that the dominant DM mechanism in our pMSSM10 analysis is chargino_1 coannihilation: {parts of its parameter space can be explored by the LHC, and a larger portion by future direct DM searches.
id cern-2040986
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2015
record_format invenio
spelling cern-20409862022-08-10T12:54:55Zdoi:10.1140/epjc/s10052-015-3718-9http://cds.cern.ch/record/2040986engBagnaschi, E.A.Buchmueller, O.Cavanaugh, R.Citron, M.De Roeck, A.Dolan, M.J.Ellis, J.R.Flächer, H.Heinemeyer, S.Isidori, G.Malik, S.Martínez Santos, D.Olive, K.A.Sakurai, K.de Vries, K.J.Weiglein, G.Supersymmetric Dark Matter after LHC Run 1Particle Physics - PhenomenologyDifferent mechanisms operate in various regions of the MSSM parameter space to bring the relic density of the lightest neutralino, neutralino_1, assumed here to be the LSP and thus the Dark Matter (DM) particle, into the range allowed by astrophysics and cosmology. These mechanisms include coannihilation with some nearly-degenerate next-to-lightest supersymmetric particle (NLSP) such as the lighter stau (stau_1), stop (stop_1) or chargino (chargino_1), resonant annihilation via direct-channel heavy Higgs bosons H/A, the light Higgs boson h or the Z boson, and enhanced annihilation via a larger Higgsino component of the LSP in the focus-point region. These mechanisms typically select lower-dimensional subspaces in MSSM scenarios such as the CMSSM, NUHM1, NUHM2 and pMSSM10. We analyze how future LHC and direct DM searches can complement each other in the exploration of the different DM mechanisms within these scenarios. We find that the stau_1 coannihilation regions of the CMSSM, NUHM1, NUHM2 can largely be explored at the LHC via searches for missing E_T events and long-lived charged particles, whereas their H/A funnel, focus-point and chargino_1 coannihilation regions can largely be explored by the LZ and Darwin DM direct detection experiments. We find that the dominant DM mechanism in our pMSSM10 analysis is chargino_1 coannihilation: {parts of its parameter space can be explored by the LHC, and a larger portion by future direct DM searches.Different mechanisms operate in various regions of the MSSM parameter space to bring the relic density of the lightest neutralino, $\tilde{\chi }^0_{1}$ , assumed here to be the lightest SUSY particle (LSP) and thus the dark matter (DM) particle, into the range allowed by astrophysics and cosmology. These mechanisms include coannihilation with some nearly degenerate next-to-lightest supersymmetric particle such as the lighter stau $\tilde{\tau }_{1}$ , stop $\tilde{t}_{1}$ or chargino $\tilde{\chi }^\pm _{1}$ , resonant annihilation via direct-channel heavy Higgs bosons H / A, the light Higgs boson h or the Z boson, and enhanced annihilation via a larger Higgsino component of the LSP in the focus-point region. These mechanisms typically select lower-dimensional subspaces in MSSM scenarios such as the CMSSM, NUHM1, NUHM2, and pMSSM10. We analyze how future LHC and direct DM searches can complement each other in the exploration of the different DM mechanisms within these scenarios. We find that the ${\tilde{\tau }_1}$ coannihilation regions of the CMSSM, NUHM1, NUHM2 can largely be explored at the LHC via searches for $/ \!\!\!\! E_T$ events and long-lived charged particles, whereas their H / A funnel, focus-point and $\tilde{\chi }^\pm _{1}$ coannihilation regions can largely be explored by the LZ and Darwin DM direct detection experiments. We find that the dominant DM mechanism in our pMSSM10 analysis is $\tilde{\chi }^\pm _{1}$ coannihilation: parts of its parameter space can be explored by the LHC, and a larger portion by future direct DM searches.Different mechanisms operate in various regions of the MSSM parameter space to bring the relic density of the lightest neutralino, neutralino $\tilde{\chi}^0_1$, assumed here to be the LSP and thus the Dark Matter (DM) particle, into the range allowed by astrophysics and cosmology. These mechanisms include coannihilation with some nearly-degenerate next-to-lightest supersymmetric particle (NLSP) such as the lighter stau ($\tilde{\tau}_1$), stop ($\tilde{t}_1$) or chargino ($\tilde{\chi}^{\pm}_1$), resonant annihilation via direct-channel heavy Higgs bosons H/A, the light Higgs boson h or the Z boson, and enhanced annihilation via a larger Higgsino component of the LSP in the focus-point region. These mechanisms typically select lower-dimensional subspaces in MSSM scenarios such as the CMSSM, NUHM1, NUHM2 and pMSSM10. We analyze how future LHC and direct DM searches can complement each other in the exploration of the different DM mechanisms within these scenarios. We find that the $\tilde{\tau}_1$ coannihilation regions of the CMSSM, NUHM1, NUHM2 can largely be explored at the LHC via searches for missing $\not E_T$ events and long-lived charged particles, whereas their H/A funnel, focus-point and $\tilde{\chi}^{\pm}_1$ coannihilation regions can largely be explored by the LZ and Darwin DM direct detection experiments. We find that the dominant DM mechanism in our pMSSM10 analysis is $\tilde{\chi}^{\pm}_1$ coannihilation: parts of its parameter space can be explored by the LHC, and a larger portion by future direct DM searches.arXiv:1508.01173KCL-PH-TH-2015-33LCTS-2015-24CERN-PH-TH-2015-167DESY-15-132FTPI-MINN-15-36UMN-TH-3445-15SLAC-PUB-16350FERMILAB-PUB-15-333-CMSKCL-PH-TH-2015-33LCTS-2015-24CERN-PH-TH-2015-167DESY 15-132FTPI-MINN-15-36UMN-TH-3445-15SLAC-PUB-16350FERMILAB-PUB-15-333-CMSoai:cds.cern.ch:20409862015-08-05
spellingShingle Particle Physics - Phenomenology
Bagnaschi, E.A.
Buchmueller, O.
Cavanaugh, R.
Citron, M.
De Roeck, A.
Dolan, M.J.
Ellis, J.R.
Flächer, H.
Heinemeyer, S.
Isidori, G.
Malik, S.
Martínez Santos, D.
Olive, K.A.
Sakurai, K.
de Vries, K.J.
Weiglein, G.
Supersymmetric Dark Matter after LHC Run 1
title Supersymmetric Dark Matter after LHC Run 1
title_full Supersymmetric Dark Matter after LHC Run 1
title_fullStr Supersymmetric Dark Matter after LHC Run 1
title_full_unstemmed Supersymmetric Dark Matter after LHC Run 1
title_short Supersymmetric Dark Matter after LHC Run 1
title_sort supersymmetric dark matter after lhc run 1
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1140/epjc/s10052-015-3718-9
http://cds.cern.ch/record/2040986
work_keys_str_mv AT bagnaschiea supersymmetricdarkmatterafterlhcrun1
AT buchmuellero supersymmetricdarkmatterafterlhcrun1
AT cavanaughr supersymmetricdarkmatterafterlhcrun1
AT citronm supersymmetricdarkmatterafterlhcrun1
AT deroecka supersymmetricdarkmatterafterlhcrun1
AT dolanmj supersymmetricdarkmatterafterlhcrun1
AT ellisjr supersymmetricdarkmatterafterlhcrun1
AT flacherh supersymmetricdarkmatterafterlhcrun1
AT heinemeyers supersymmetricdarkmatterafterlhcrun1
AT isidorig supersymmetricdarkmatterafterlhcrun1
AT maliks supersymmetricdarkmatterafterlhcrun1
AT martinezsantosd supersymmetricdarkmatterafterlhcrun1
AT oliveka supersymmetricdarkmatterafterlhcrun1
AT sakuraik supersymmetricdarkmatterafterlhcrun1
AT devrieskj supersymmetricdarkmatterafterlhcrun1
AT weigleing supersymmetricdarkmatterafterlhcrun1