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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...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1997
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/S0550-3213(98)00417-9 http://cds.cern.ch/record/687512 |
_version_ | 1780901768556707840 |
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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 |