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Search for the Next-To-Lightest Neutralino

We study the inclusive production of the next-to-lightest neutralino decaying directly, or via slepton, into two leptons and the lightest neutralino. Events are selected in the inclusive 3 lepton or 3 lepton + ET missing final states. The study is carried out in the framework of the minimal SUGRA mo...

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Detalles Bibliográficos
Autores principales: Iashvili, Ia, Kharchilava, Avto
Lenguaje:eng
Publicado: 1997
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(98)00417-9
http://cds.cern.ch/record/687512
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author Iashvili, Ia
Kharchilava, Avto
author_facet Iashvili, Ia
Kharchilava, Avto
author_sort Iashvili, Ia
collection CERN
description We study the inclusive production of the next-to-lightest neutralino decaying directly, or via slepton, into two leptons and the lightest neutralino. Events are selected in the inclusive 3 lepton or 3 lepton + ET missing final states. The study is carried out in the framework of the minimal SUGRA model with one set of parameters: tan( beta)=2, A0=0, mu<0. The region of ( m0, m1/2) parameter space, where the next-to-lightest neutralino is observable by the characteristic shape of the dilepton invariant mass spectrum, is delineated. The possibilities to determine the model parameters through the measurement of neutralinos and slepton masses are discussed.
id cern-687512
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1997
record_format invenio
spelling cern-6875122019-09-30T06:29:59Zdoi:10.1016/S0550-3213(98)00417-9http://cds.cern.ch/record/687512engIashvili, IaKharchilava, AvtoSearch for the Next-To-Lightest NeutralinoDetectors and Experimental TechniquesParticle Physics - PhenomenologyWe study the inclusive production of the next-to-lightest neutralino decaying directly, or via slepton, into two leptons and the lightest neutralino. Events are selected in the inclusive 3 lepton or 3 lepton + ET missing final states. The study is carried out in the framework of the minimal SUGRA model with one set of parameters: tan( beta)=2, A0=0, mu<0. The region of ( m0, m1/2) parameter space, where the next-to-lightest neutralino is observable by the characteristic shape of the dilepton invariant mass spectrum, is delineated. The possibilities to determine the model parameters through the measurement of neutralinos and slepton masses are discussed.hep-ph/9712393CMS-NOTE-1997-065oai:cds.cern.ch:6875121997-08-08
spellingShingle Detectors and Experimental Techniques
Particle Physics - Phenomenology
Iashvili, Ia
Kharchilava, Avto
Search for the Next-To-Lightest Neutralino
title Search for the Next-To-Lightest Neutralino
title_full Search for the Next-To-Lightest Neutralino
title_fullStr Search for the Next-To-Lightest Neutralino
title_full_unstemmed Search for the Next-To-Lightest Neutralino
title_short Search for the Next-To-Lightest Neutralino
title_sort search for the next-to-lightest neutralino
topic Detectors and Experimental Techniques
Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(98)00417-9
http://cds.cern.ch/record/687512
work_keys_str_mv AT iashviliia searchforthenexttolightestneutralino
AT kharchilavaavto searchforthenexttolightestneutralino