Cargando…
On the detectability of the CMSSM light Higgs boson at the Tevatron
We examine the prospects of detecting the light Higgs scalar h^0 of the Constrained MSSM at the Tevatron. To this end we explore large ranges of the CMSSM parameter space with mu>0 using a Markov Chain Monte Carlo technique, and apply all relevant collider and cosmological constraints including t...
Autores principales: | , , |
---|---|
Lenguaje: | eng |
Publicado: |
2006
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/1126-6708/2007/04/084 http://cds.cern.ch/record/998665 |
_version_ | 1780911546014105600 |
---|---|
author | Roszkowski, Leszek Ruiz de Austri, Roberto Trotta, Roberto |
author_facet | Roszkowski, Leszek Ruiz de Austri, Roberto Trotta, Roberto |
author_sort | Roszkowski, Leszek |
collection | CERN |
description | We examine the prospects of detecting the light Higgs scalar h^0 of the Constrained MSSM at the Tevatron. To this end we explore large ranges of the CMSSM parameter space with mu>0 using a Markov Chain Monte Carlo technique, and apply all relevant collider and cosmological constraints including their uncertainties, as well as those of the Standard Model parameters. Using the formalism of Bayesian statistics we find that the 68% posterior probability region for the light Higgs mass lies between 116.0 GeV and 120.4 GeV. Otherwise, h^0 is very similar to the Standard Model Higgs boson. Nevertheless, we point out some enhancements in its couplings to bottom and tau pairs, ranging from a few per cent in most of the CMSSM parameter space, up to several per cent in the most favored region of tan(beta)~50 and the pseudoscalar Higgs mass of m_A~1 TeV. We also find that the other Higgs bosons are typically too heavy to be produced at the Tevatron. We conclude that, over the whole CMSSM light Higgs 95% posterior probability mass range, a 95% CL exclusion limit can be set with about 2/fb of integrated luminosity per experiment, or else with 4/fb (12/fb) a 3 sigma evidence (5 sigma discovery) will be guaranteed. We also emphasize that the alternative measure of the mean quality of fit favors a somewhat lower Higgs mass range; this implies even more optimistic prospects for the CMSSM light Higgs search than with the more conservative Bayesian approach. In conclusion, at the Tevatron either some evidence will be found for the light Higgs boson or, at a high confidence level, the CMSSM will be ruled out. |
id | cern-998665 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2006 |
record_format | invenio |
spelling | cern-9986652022-04-19T06:05:16Zdoi:10.1088/1126-6708/2007/04/084http://cds.cern.ch/record/998665engRoszkowski, LeszekRuiz de Austri, RobertoTrotta, RobertoOn the detectability of the CMSSM light Higgs boson at the TevatronParticle Physics - PhenomenologyWe examine the prospects of detecting the light Higgs scalar h^0 of the Constrained MSSM at the Tevatron. To this end we explore large ranges of the CMSSM parameter space with mu>0 using a Markov Chain Monte Carlo technique, and apply all relevant collider and cosmological constraints including their uncertainties, as well as those of the Standard Model parameters. Using the formalism of Bayesian statistics we find that the 68% posterior probability region for the light Higgs mass lies between 116.0 GeV and 120.4 GeV. Otherwise, h^0 is very similar to the Standard Model Higgs boson. Nevertheless, we point out some enhancements in its couplings to bottom and tau pairs, ranging from a few per cent in most of the CMSSM parameter space, up to several per cent in the most favored region of tan(beta)~50 and the pseudoscalar Higgs mass of m_A~1 TeV. We also find that the other Higgs bosons are typically too heavy to be produced at the Tevatron. We conclude that, over the whole CMSSM light Higgs 95% posterior probability mass range, a 95% CL exclusion limit can be set with about 2/fb of integrated luminosity per experiment, or else with 4/fb (12/fb) a 3 sigma evidence (5 sigma discovery) will be guaranteed. We also emphasize that the alternative measure of the mean quality of fit favors a somewhat lower Higgs mass range; this implies even more optimistic prospects for the CMSSM light Higgs search than with the more conservative Bayesian approach. In conclusion, at the Tevatron either some evidence will be found for the light Higgs boson or, at a high confidence level, the CMSSM will be ruled out.We examine the prospects of detecting the light Higgs h^0 of the Constrained MSSM at the Tevatron. To this end we explore the CMSSM parameter space with \mu>0, using a Markov Chain Monte Carlo technique, and apply all relevant collider and cosmological constraints including their uncertainties, as well as those of the Standard Model parameters. Taking 50 GeV < m_{1/2}, m_0 < 4 TeV, |A_0| < 7 TeV and 2 < tan(beta) < 62 as flat priors and using the formalism of Bayesian statistics we find that the 68% posterior probability region for the h^0 mass lies between 115.4 GeV and 120.4 GeV. Otherwise, h^0 is very similar to the Standard Model Higgs boson. Nevertheless, we point out some enhancements in its couplings to bottom and tau pairs, ranging from a few per cent in most of the CMSSM parameter space, up to several per cent in the favored region of tan(beta)\sim 50 and the pseudoscalar Higgs mass of m_A\lsim 1 TeV. We also find that the other Higgs bosons are typically heavier, although not necessarily much heavier. For values of the CMSSM light Higgs mass within the 95% probability range as determined by our analysis, a 95% CL exclusion limit can be set with about 2/fb of integrated luminosity per experiment, or else with 4/fb (12/fb) a 3 sigma evidence (5 sigma discovery) will be guaranteed. We also emphasize that the alternative statistical measure of the mean quality-of-fit favors a somewhat lower Higgs mass range: this implies even more optimistic prospects for the CMSSM light Higgs search than the more conservative Bayesian approach. In conclusion, for the above CMSSM parameter ranges, either some evidence will be found at the Tevatron for the light Higgs boson or, at a high confidence level, the CMSSM will be ruled out.hep-ph/0611173CERN-PH-TH-2006-224CERN-PH-TH-2006-224oai:cds.cern.ch:9986652006-11-13 |
spellingShingle | Particle Physics - Phenomenology Roszkowski, Leszek Ruiz de Austri, Roberto Trotta, Roberto On the detectability of the CMSSM light Higgs boson at the Tevatron |
title | On the detectability of the CMSSM light Higgs boson at the Tevatron |
title_full | On the detectability of the CMSSM light Higgs boson at the Tevatron |
title_fullStr | On the detectability of the CMSSM light Higgs boson at the Tevatron |
title_full_unstemmed | On the detectability of the CMSSM light Higgs boson at the Tevatron |
title_short | On the detectability of the CMSSM light Higgs boson at the Tevatron |
title_sort | on the detectability of the cmssm light higgs boson at the tevatron |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1088/1126-6708/2007/04/084 http://cds.cern.ch/record/998665 |
work_keys_str_mv | AT roszkowskileszek onthedetectabilityofthecmssmlighthiggsbosonatthetevatron AT ruizdeaustriroberto onthedetectabilityofthecmssmlighthiggsbosonatthetevatron AT trottaroberto onthedetectabilityofthecmssmlighthiggsbosonatthetevatron |