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Testing SUSY at the LHC: Electroweak and Dark matter fine tuning at two-loop order

In the framework of the Constrained Minimal Supersymmetric Standard Model (CMSSM) we evaluate the electroweak fine tuning measure that provides a quantitative test of supersymmetry as a solution to the hierarchy problem. Taking account of current experimental constraints we compute the fine tuning a...

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Autores principales: Cassel, S., Ghilencea, D.M., Ross, G.G.
Formato: info:eu-repo/semantics/article
Lenguaje:eng
Publicado: Nucl. Phys. B 2010
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2010.03.031
http://cds.cern.ch/record/1235198
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author Cassel, S.
Ghilencea, D.M.
Ross, G.G.
author_facet Cassel, S.
Ghilencea, D.M.
Ross, G.G.
author_sort Cassel, S.
collection CERN
description In the framework of the Constrained Minimal Supersymmetric Standard Model (CMSSM) we evaluate the electroweak fine tuning measure that provides a quantitative test of supersymmetry as a solution to the hierarchy problem. Taking account of current experimental constraints we compute the fine tuning at two-loop order and determine the limits on the CMSSM parameter space and the measurements at the LHC most relevant in covering it. Without imposing the LEPII bound on the Higgs mass, it is shown that the fine tuning computed at two-loop has a minimum $\Delta=8.8$ corresponding to a Higgs mass $m_h=114\pm 2$ GeV. Adding the constraint that the SUSY dark matter relic density should be within present bounds we find $\Delta=15$ corresponding to $m_h=114.7\pm 2$ GeV and this rises to $\Delta=17.8$ ($m_h=115.9\pm 2$ GeV) for SUSY dark matter abundance within 3$\sigma$ of the WMAP constraint. We extend the analysis to include the contribution of dark matter fine tuning. In this case the overall fine tuning and Higgs mass are only marginally larger for the case SUSY dark matter is subdominant and rises to $\Delta=28.7$ ($m_h=116.98\pm 2$ GeV) for the case of SUSY dark matter saturates the WMAP bound. For a Higgs mass above these values, fine tuning rises exponentially fast. The CMSSM spectrum that corresponds to minimal fine tuning is computed and provides a benchmark for future searches. It is characterised by heavy squarks and sleptons a nd light neutralinos, charginos and gluinos.
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spelling cern-12351982023-03-12T05:20:11Z doi:10.1016/j.nuclphysb.2010.03.031 http://cds.cern.ch/record/1235198 eng Cassel, S. Ghilencea, D.M. Ross, G.G. Testing SUSY at the LHC: Electroweak and Dark matter fine tuning at two-loop order Particle Physics - Phenomenology In the framework of the Constrained Minimal Supersymmetric Standard Model (CMSSM) we evaluate the electroweak fine tuning measure that provides a quantitative test of supersymmetry as a solution to the hierarchy problem. Taking account of current experimental constraints we compute the fine tuning at two-loop order and determine the limits on the CMSSM parameter space and the measurements at the LHC most relevant in covering it. Without imposing the LEPII bound on the Higgs mass, it is shown that the fine tuning computed at two-loop has a minimum $\Delta=8.8$ corresponding to a Higgs mass $m_h=114\pm 2$ GeV. Adding the constraint that the SUSY dark matter relic density should be within present bounds we find $\Delta=15$ corresponding to $m_h=114.7\pm 2$ GeV and this rises to $\Delta=17.8$ ($m_h=115.9\pm 2$ GeV) for SUSY dark matter abundance within 3$\sigma$ of the WMAP constraint. We extend the analysis to include the contribution of dark matter fine tuning. In this case the overall fine tuning and Higgs mass are only marginally larger for the case SUSY dark matter is subdominant and rises to $\Delta=28.7$ ($m_h=116.98\pm 2$ GeV) for the case of SUSY dark matter saturates the WMAP bound. For a Higgs mass above these values, fine tuning rises exponentially fast. The CMSSM spectrum that corresponds to minimal fine tuning is computed and provides a benchmark for future searches. It is characterised by heavy squarks and sleptons a nd light neutralinos, charginos and gluinos. In the framework of the Constrained Minimal Supersymmetric Standard Model (CMSSM) we evaluate the electroweak fine tuning measure that provides a quantitative test of supersymmetry as a solution to the hierarchy problem. Taking account of current experimental constraints we compute the fine tuning at two-loop order and determine the limits on the CMSSM parameter space and the measurements at the LHC most relevant in covering it. Without imposing the LEPII bound on the Higgs mass, it is shown that the fine tuning computed at two-loop has a minimum Δ = 8.8 corresponding to a Higgs mass m h = 114 ± 2 GeV . Adding the constraint that the SUSY dark matter relic density should be within present bounds we find Δ = 15 corresponding to m h = 114.7 ± 2 GeV and this rises to Δ = 17.8 ( m h = 115.9 ± 2 GeV ) for SUSY dark matter abundance within 3 σ of the WMAP constraint. We extend the analysis to include the contribution of dark matter fine tuning. In this case the overall fine tuning and Higgs mass are only marginally larger for the case SUSY dark matter is subdominant and rises to Δ = 28.7 ( m h = 116.98 ± 2 GeV ) for the case of SUSY dark matter saturates the WMAP bound. For a Higgs mass above these values, fine tuning rises exponentially fast. The CMSSM spectrum that corresponds to minimal fine tuning is computed and provides a benchmark for future searches. It is characterised by heavy squarks and sleptons and light neutralinos, charginos and gluinos. In the framework of the Constrained Minimal Supersymmetric Standard Model (CMSSM) we evaluate the electroweak fine tuning measure that provides a quantitative test of supersymmetry as a solution to the hierarchy problem. Taking account of current experimental constraints we compute the fine tuning at two-loop order and determine the limits on the CMSSM parameter space and the measurements at the LHC most relevant in covering it. Without imposing the LEPII bound on the Higgs mass, it is shown that the fine tuning computed at two-loop has a minimum $\Delta=8.8$ corresponding to a Higgs mass $m_h=114\pm 2$ GeV. Adding the constraint that the SUSY dark matter relic density should be within present bounds we find $\Delta=15$ corresponding to $m_h=114.7\pm 2$ GeV and this rises to $\Delta=17.8$ ($m_h=115.9\pm 2$ GeV) for SUSY dark matter abundance within 3$\sigma$ of the WMAP constraint. We extend the analysis to include the contribution of dark matter fine tuning. In this case the overall fine tuning and Higgs mass are only marginally larger for the case SUSY dark matter is subdominant and rises to $\Delta=28.7$ ($m_h=116.98\pm 2$ GeV) for the case of SUSY dark matter saturates the WMAP bound. For a Higgs mass above these values, fine tuning rises exponentially fast. The CMSSM spectrum that corresponds to minimal fine tuning is computed and provides a benchmark for future searches. It is characterised by heavy squarks and sleptons and light neutralinos, charginos and gluinos. info:eu-repo/grantAgreement/EC/FP7/226371 info:eu-repo/semantics/openAccess Education Level info:eu-repo/semantics/article info:eu-repo/grantAgreement/EC/FP7/237920 info:eu-repo/semantics/openAccess Education Level info:eu-repo/semantics/article http://cds.cern.ch/record/1235198 Nucl. Phys. B Nucl. Phys. B, (2010) pp. 110-134 2010-01-25
spellingShingle Particle Physics - Phenomenology
Cassel, S.
Ghilencea, D.M.
Ross, G.G.
Testing SUSY at the LHC: Electroweak and Dark matter fine tuning at two-loop order
title Testing SUSY at the LHC: Electroweak and Dark matter fine tuning at two-loop order
title_full Testing SUSY at the LHC: Electroweak and Dark matter fine tuning at two-loop order
title_fullStr Testing SUSY at the LHC: Electroweak and Dark matter fine tuning at two-loop order
title_full_unstemmed Testing SUSY at the LHC: Electroweak and Dark matter fine tuning at two-loop order
title_short Testing SUSY at the LHC: Electroweak and Dark matter fine tuning at two-loop order
title_sort testing susy at the lhc: electroweak and dark matter fine tuning at two-loop order
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.nuclphysb.2010.03.031
http://cds.cern.ch/record/1235198
http://cds.cern.ch/record/1235198
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