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Dirac Triplet Extension of the MSSM

In this paper we explore extensions of the Minimal Supersymmetric Standard Model involving two $SU(2)_L$ triplet chiral superfields that share a superpotential Dirac mass yet only one of which couples to the Higgs fields. This choice is motivated by recent work using two singlet superfields with the...

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Detalles Bibliográficos
Autores principales: Alvarado, C., Delgado, Antonio, Martin, A., Ostdiek, B.
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.92.035009
http://cds.cern.ch/record/2009283
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author Alvarado, C.
Delgado, Antonio
Martin, A.
Ostdiek, B.
author_facet Alvarado, C.
Delgado, Antonio
Martin, A.
Ostdiek, B.
author_sort Alvarado, C.
collection CERN
description In this paper we explore extensions of the Minimal Supersymmetric Standard Model involving two $SU(2)_L$ triplet chiral superfields that share a superpotential Dirac mass yet only one of which couples to the Higgs fields. This choice is motivated by recent work using two singlet superfields with the same superpotential requirements. We find that, as in the singlet case, the Higgs mass in the triplet extension can easily be raised to $125\,\text{GeV}$ without introducing large fine-tuning. For triplets that carry hypercharge, the regions of least fine tuning are characterized by small contributions to the $\mathcal T$ parameter, and light stop squarks, $m_{\tilde t_1} \sim 300-450\,\text{GeV}$; the latter is a result of the $\tan\beta$ dependence of the triplet contribution to the Higgs mass. Despite such light stop masses, these models are viable provided the stop-electroweakino spectrum is sufficiently compressed.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2015
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spelling cern-20092832022-08-13T02:25:10Zdoi:10.1103/PhysRevD.92.035009http://cds.cern.ch/record/2009283engAlvarado, C.Delgado, AntonioMartin, A.Ostdiek, B.Dirac Triplet Extension of the MSSMParticle Physics - PhenomenologyIn this paper we explore extensions of the Minimal Supersymmetric Standard Model involving two $SU(2)_L$ triplet chiral superfields that share a superpotential Dirac mass yet only one of which couples to the Higgs fields. This choice is motivated by recent work using two singlet superfields with the same superpotential requirements. We find that, as in the singlet case, the Higgs mass in the triplet extension can easily be raised to $125\,\text{GeV}$ without introducing large fine-tuning. For triplets that carry hypercharge, the regions of least fine tuning are characterized by small contributions to the $\mathcal T$ parameter, and light stop squarks, $m_{\tilde t_1} \sim 300-450\,\text{GeV}$; the latter is a result of the $\tan\beta$ dependence of the triplet contribution to the Higgs mass. Despite such light stop masses, these models are viable provided the stop-electroweakino spectrum is sufficiently compressed.In this paper we explore extensions of the minimal supersymmetric standard model involving two SU(2)L triplet chiral superfields that share a superpotential Dirac mass, only one of which couples to the Higgs fields. This choice is motivated by recent work using two singlet superfields with the same superpotential requirements. We find that, as in the singlet case, the Higgs mass in the triplet extension can easily be raised to 125 GeV without introducing large fine-tuning. For triplets that carry hypercharge, the regions of least fine-tuning are characterized by small contributions to the T parameter, and light stop squarks, mt˜1∼300-450  GeV; the latter is a result of the tanβ dependence of the triplet contribution to the Higgs mass. Despite such light stop masses, these models are viable provided the stop-electroweakino spectrum is sufficiently compressed.In this paper we explore extensions of the Minimal Supersymmetric Standard Model involving two $SU(2)_L$ triplet chiral superfields that share a superpotential Dirac mass yet only one of which couples to the Higgs fields. This choice is motivated by recent work using two singlet superfields with the same superpotential requirements. We find that, as in the singlet case, the Higgs mass in the triplet extension can easily be raised to $125\,\text{GeV}$ without introducing large fine-tuning. For triplets that carry hypercharge, the regions of least fine tuning are characterized by small contributions to the $\mathcal T$ parameter, and light stop squarks, $m_{\tilde t_1} \sim 300-450\,\text{GeV}$; the latter is a result of the $\tan\beta$ dependence of the triplet contribution to the Higgs mass. Despite such light stop masses, these models are viable provided the stop-electroweakino spectrum is sufficiently compressed.arXiv:1504.03683CERN-PH-TH-2015-084CERN-PH-TH-2015-084oai:cds.cern.ch:20092832015-04-14
spellingShingle Particle Physics - Phenomenology
Alvarado, C.
Delgado, Antonio
Martin, A.
Ostdiek, B.
Dirac Triplet Extension of the MSSM
title Dirac Triplet Extension of the MSSM
title_full Dirac Triplet Extension of the MSSM
title_fullStr Dirac Triplet Extension of the MSSM
title_full_unstemmed Dirac Triplet Extension of the MSSM
title_short Dirac Triplet Extension of the MSSM
title_sort dirac triplet extension of the mssm
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.92.035009
http://cds.cern.ch/record/2009283
work_keys_str_mv AT alvaradoc diractripletextensionofthemssm
AT delgadoantonio diractripletextensionofthemssm
AT martina diractripletextensionofthemssm
AT ostdiekb diractripletextensionofthemssm