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Singular ways to search for the Higgs boson
The discovery or exclusion of the fundamental standard scalar is a hot topic, given the data of LEP, the Tevatron and the LHC, as well as the advanced status of the pertinent theoretical calculations. With the current statistics at the hadron colliders, the workhorse decay channel, at all relevant H...
Autores principales: | , |
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Lenguaje: | eng |
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2012
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Acceso en línea: | https://dx.doi.org/10.1007/JHEP06(2012)091 http://cds.cern.ch/record/1423826 |
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author | De Rujula, A. Galindo, A. |
author_facet | De Rujula, A. Galindo, A. |
author_sort | De Rujula, A. |
collection | CERN |
description | The discovery or exclusion of the fundamental standard scalar is a hot topic, given the data of LEP, the Tevatron and the LHC, as well as the advanced status of the pertinent theoretical calculations. With the current statistics at the hadron colliders, the workhorse decay channel, at all relevant H masses, is H to WW, followed by W to light leptons. Using phase-space singularity techniques, we construct and study a plethora of "singularity variables" meant to facilitate the difficult tasks of separating signal and backgrounds and of measuring the mass of a putative signal. The simplest singularity variables are not invariant under boosts along the collider's axes and the simulation of their distributions requires a good understanding of parton distribution functions, perhaps not a serious shortcoming during the boson hunting season. The derivation of longitudinally boost-invariant variables, which are functions of the four charged-lepton observables that share this invariance, is quite elaborate. But their use is simple and they are, in a kinematical sense, optimal. |
id | cern-1423826 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2012 |
record_format | invenio |
spelling | cern-14238262023-03-14T17:27:30Zdoi:10.1007/JHEP06(2012)091http://cds.cern.ch/record/1423826engDe Rujula, A.Galindo, A.Singular ways to search for the Higgs bosonParticle Physics - PhenomenologyThe discovery or exclusion of the fundamental standard scalar is a hot topic, given the data of LEP, the Tevatron and the LHC, as well as the advanced status of the pertinent theoretical calculations. With the current statistics at the hadron colliders, the workhorse decay channel, at all relevant H masses, is H to WW, followed by W to light leptons. Using phase-space singularity techniques, we construct and study a plethora of "singularity variables" meant to facilitate the difficult tasks of separating signal and backgrounds and of measuring the mass of a putative signal. The simplest singularity variables are not invariant under boosts along the collider's axes and the simulation of their distributions requires a good understanding of parton distribution functions, perhaps not a serious shortcoming during the boson hunting season. The derivation of longitudinally boost-invariant variables, which are functions of the four charged-lepton observables that share this invariance, is quite elaborate. But their use is simple and they are, in a kinematical sense, optimal.The discovery or exclusion of the fundamental standard scalar is a hot topic, given the data of LEP, the Tevatron and the LHC, as well as the advanced status of the pertinent theoretical calculations. With the current statistics at the hadron colliders, the workhorse decay channel, at all relevant H masses, is H to WW, followed by W to light leptons. Using phase-space singularity techniques, we construct and study a plethora of "singularity variables" meant to facilitate the difficult tasks of separating signal and backgrounds and of measuring the mass of a putative signal. The simplest singularity variables are not invariant under boosts along the collider's axes and the simulation of their distributions requires a good understanding of parton distribution functions, perhaps not a serious shortcoming during the boson hunting season. The derivation of longitudinally boost-invariant variables, which are functions of the four charged-lepton observables that share this invariance, is quite elaborate. But their use is simple and they are, in a kinematical sense, optimal.arXiv:1202.2552CERN-PH-TH-2012-039CERN-PH-TH-2012-039oai:cds.cern.ch:14238262012-02-14 |
spellingShingle | Particle Physics - Phenomenology De Rujula, A. Galindo, A. Singular ways to search for the Higgs boson |
title | Singular ways to search for the Higgs boson |
title_full | Singular ways to search for the Higgs boson |
title_fullStr | Singular ways to search for the Higgs boson |
title_full_unstemmed | Singular ways to search for the Higgs boson |
title_short | Singular ways to search for the Higgs boson |
title_sort | singular ways to search for the higgs boson |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP06(2012)091 http://cds.cern.ch/record/1423826 |
work_keys_str_mv | AT derujulaa singularwaystosearchforthehiggsboson AT galindoa singularwaystosearchforthehiggsboson |