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Prediction for the Lightest Higgs Boson Mass in the CMSSM using Indirect Experimental Constraints

Measurements at low energies provide interesting indirect information about masses of particles that are (so far) too heavy to be produced directly. Motivated by recent progress in consistently and rigorously calculating electroweak precision observables and flavour related observables, we derive th...

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Detalles Bibliográficos
Autores principales: Buchmueller, O., Cavanaugh, R., De Roeck, A., Heinemeyer, S., Isidori, G., Paradisi, P., Ronga, F.J., Weber, A.M., Weiglein, G.
Lenguaje:eng
Publicado: 2007
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2007.09.058
http://cds.cern.ch/record/1157244
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author Buchmueller, O.
Cavanaugh, R.
De Roeck, A.
Heinemeyer, S.
Isidori, G.
Paradisi, P.
Ronga, F.J.
Weber, A.M.
Weiglein, G.
author_facet Buchmueller, O.
Cavanaugh, R.
De Roeck, A.
Heinemeyer, S.
Isidori, G.
Paradisi, P.
Ronga, F.J.
Weber, A.M.
Weiglein, G.
author_sort Buchmueller, O.
collection CERN
description Measurements at low energies provide interesting indirect information about masses of particles that are (so far) too heavy to be produced directly. Motivated by recent progress in consistently and rigorously calculating electroweak precision observables and flavour related observables, we derive the *preferred* value for m_h in the Constrained Minimal Supersymmetric Standard Model (CMSSM), obtained from a fit taking into account electroweak precision data, flavour physics observables and the abundance of Cold Dark Matter. No restriction is imposed on m_h itself: the experimental bound from direct Higgs boson search at LEP is not included in the fit. A multi-parameter chi^2 is minimized with respect to the free parameters of the CMSSM, M_0, $M_(1/2)$, A_0, tan\beta. A statistical comparison with the Standard Model fit to the electroweak precision data is made. The preferred value for the lightest Higgs boson mass in the CMSSM is found to be $m_h^(CMSSM)$ = $110^+8_-10$(exp.)+-3(theo.) GeV/c^2, where the first uncertainty is experimental and the second uncertainty is theoretical. This value is compatible with the limit from direct Higgs boson search at LEP.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2007
record_format invenio
spelling cern-11572442023-03-14T19:18:41Zdoi:10.1016/j.physletb.2007.09.058http://cds.cern.ch/record/1157244engBuchmueller, O.Cavanaugh, R.De Roeck, A.Heinemeyer, S.Isidori, G.Paradisi, P.Ronga, F.J.Weber, A.M.Weiglein, G.Prediction for the Lightest Higgs Boson Mass in the CMSSM using Indirect Experimental ConstraintsParticle Physics - PhenomenologyParticle Physics - ExperimentMeasurements at low energies provide interesting indirect information about masses of particles that are (so far) too heavy to be produced directly. Motivated by recent progress in consistently and rigorously calculating electroweak precision observables and flavour related observables, we derive the *preferred* value for m_h in the Constrained Minimal Supersymmetric Standard Model (CMSSM), obtained from a fit taking into account electroweak precision data, flavour physics observables and the abundance of Cold Dark Matter. No restriction is imposed on m_h itself: the experimental bound from direct Higgs boson search at LEP is not included in the fit. A multi-parameter chi^2 is minimized with respect to the free parameters of the CMSSM, M_0, $M_(1/2)$, A_0, tan\beta. A statistical comparison with the Standard Model fit to the electroweak precision data is made. The preferred value for the lightest Higgs boson mass in the CMSSM is found to be $m_h^(CMSSM)$ = $110^+8_-10$(exp.)+-3(theo.) GeV/c^2, where the first uncertainty is experimental and the second uncertainty is theoretical. This value is compatible with the limit from direct Higgs boson search at LEP.Measurements at low energies provide interesting indirect information about masses of particles that are (so far) too heavy to be produced directly. Motivated by recent progress in consistently and rigorously calculating electroweak precision observables and flavour related observables, we derive the preferred value for mh in the Constrained Minimal Supersymmetric Standard Model (CMSSM), obtained from a fit taking into account electroweak precision data, flavour physics observables and the abundance of cold dark matter. No restriction is imposed on mh itself: the experimental bound from direct Higgs boson search at LEP is not included in the fit. A multi-parameter χ2 is minimized with respect to the free parameters of the CMSSM, M0 , M1/2 , A0 , tanβ . A statistical comparison with the Standard Model fit to the electroweak precision data is made. The preferred value for the lightest Higgs boson mass in the CMSSM is found to be mhCMSSM=110−10+8(exp.)±3(theo.) GeV/c2 , where the first uncertainty is experimental and the second uncertainty is theoretical. This value is compatible with the limit from direct Higgs boson search at LEP.Measurements at low energies provide interesting indirect information about masses of particles that are (so far) too heavy to be produced directly. Motivated by recent progress in consistently and rigorously calculating electroweak precision observables and flavour related observables, we derive the preferred value for m_h in the Constrained Minimal Supersymmetric Standard Model (CMSSM), obtained from a fit taking into account electroweak precision data, flavour physics observables and the abundance of Cold Dark Matter. No restriction is imposed on m_h itself: the experimental bound from direct Higgs boson search at LEP is not included in the fit. A multi-parameter chi^2 is minimized with respect to the free parameters of the CMSSM, M_0, M_1/2, A_0, tan(beta). A statistical comparison with the Standard Model fit to the electroweak precision data is made. The preferred value for the lightest Higgs boson mass in the CMSSM is found to be m_h^CMSSM = 110+8-10(exp.)+-3(theo.) GeV/c^2, where the first uncertainty is experimental and the second uncertainty is theoretical. This value is in agreement with the limit from direct Higgs boson search at LEP.arXiv:0707.3447CERN-PH-EP-2007-037oai:cds.cern.ch:11572442007-09-27
spellingShingle Particle Physics - Phenomenology
Particle Physics - Experiment
Buchmueller, O.
Cavanaugh, R.
De Roeck, A.
Heinemeyer, S.
Isidori, G.
Paradisi, P.
Ronga, F.J.
Weber, A.M.
Weiglein, G.
Prediction for the Lightest Higgs Boson Mass in the CMSSM using Indirect Experimental Constraints
title Prediction for the Lightest Higgs Boson Mass in the CMSSM using Indirect Experimental Constraints
title_full Prediction for the Lightest Higgs Boson Mass in the CMSSM using Indirect Experimental Constraints
title_fullStr Prediction for the Lightest Higgs Boson Mass in the CMSSM using Indirect Experimental Constraints
title_full_unstemmed Prediction for the Lightest Higgs Boson Mass in the CMSSM using Indirect Experimental Constraints
title_short Prediction for the Lightest Higgs Boson Mass in the CMSSM using Indirect Experimental Constraints
title_sort prediction for the lightest higgs boson mass in the cmssm using indirect experimental constraints
topic Particle Physics - Phenomenology
Particle Physics - Experiment
url https://dx.doi.org/10.1016/j.physletb.2007.09.058
http://cds.cern.ch/record/1157244
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