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Combined limits on the number of light neutrinos and the top mass from measurement of R=$\sigma$ ( W -> $\ell \nu$) / $\sigma$ ( Z -> $\ell \ell$)

Using the recent measurement of the ratio ofW→ℓv toZ→ℓℓ partial production cross-sections by UA1 and UA2, we derive an upper limit on the number of neutrinos and on the top quark mass, in the framework of the minimal standard model. To reduce the uncertainty on these limits, we use the most recent d...

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Detalles Bibliográficos
Autores principales: Colas, P, Denegri, Daniel, Stubenrauch, C
Lenguaje:eng
Publicado: 1988
Materias:
Acceso en línea:http://cds.cern.ch/record/972654
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author Colas, P
Denegri, Daniel
Stubenrauch, C
author_facet Colas, P
Denegri, Daniel
Stubenrauch, C
author_sort Colas, P
collection CERN
description Using the recent measurement of the ratio ofW→ℓv toZ→ℓℓ partial production cross-sections by UA1 and UA2, we derive an upper limit on the number of neutrinos and on the top quark mass, in the framework of the minimal standard model. To reduce the uncertainty on these limits, we use the most recent determination of sin2 θ w and the latest measurements of the structure functions by muon deep-inelastic experiments. No limit onm top is obtained in the case of three neutrino families at the 95% C.L., while a fourth generation is excluded at this confidence level if the top mass is higher thanM w −m b and if there is no new heavy lepton contribution in theW decay. The implications of light fourth generationb' andL are also investigated.
id cern-972654
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1988
record_format invenio
spelling cern-9726542019-09-30T06:29:59Zhttp://cds.cern.ch/record/972654engColas, PDenegri, DanielStubenrauch, CCombined limits on the number of light neutrinos and the top mass from measurement of R=$\sigma$ ( W -> $\ell \nu$) / $\sigma$ ( Z -> $\ell \ell$)Particle Physics - PhenomenologyUsing the recent measurement of the ratio ofW→ℓv toZ→ℓℓ partial production cross-sections by UA1 and UA2, we derive an upper limit on the number of neutrinos and on the top quark mass, in the framework of the minimal standard model. To reduce the uncertainty on these limits, we use the most recent determination of sin2 θ w and the latest measurements of the structure functions by muon deep-inelastic experiments. No limit onm top is obtained in the case of three neutrino families at the 95% C.L., while a fourth generation is excluded at this confidence level if the top mass is higher thanM w −m b and if there is no new heavy lepton contribution in theW decay. The implications of light fourth generationb' andL are also investigated.CERN-EP-88-16SACLAY-DPHPE-88-02oai:cds.cern.ch:9726541988-02-11
spellingShingle Particle Physics - Phenomenology
Colas, P
Denegri, Daniel
Stubenrauch, C
Combined limits on the number of light neutrinos and the top mass from measurement of R=$\sigma$ ( W -> $\ell \nu$) / $\sigma$ ( Z -> $\ell \ell$)
title Combined limits on the number of light neutrinos and the top mass from measurement of R=$\sigma$ ( W -> $\ell \nu$) / $\sigma$ ( Z -> $\ell \ell$)
title_full Combined limits on the number of light neutrinos and the top mass from measurement of R=$\sigma$ ( W -> $\ell \nu$) / $\sigma$ ( Z -> $\ell \ell$)
title_fullStr Combined limits on the number of light neutrinos and the top mass from measurement of R=$\sigma$ ( W -> $\ell \nu$) / $\sigma$ ( Z -> $\ell \ell$)
title_full_unstemmed Combined limits on the number of light neutrinos and the top mass from measurement of R=$\sigma$ ( W -> $\ell \nu$) / $\sigma$ ( Z -> $\ell \ell$)
title_short Combined limits on the number of light neutrinos and the top mass from measurement of R=$\sigma$ ( W -> $\ell \nu$) / $\sigma$ ( Z -> $\ell \ell$)
title_sort combined limits on the number of light neutrinos and the top mass from measurement of r=$\sigma$ ( w -> $\ell \nu$) / $\sigma$ ( z -> $\ell \ell$)
topic Particle Physics - Phenomenology
url http://cds.cern.ch/record/972654
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AT denegridaniel combinedlimitsonthenumberoflightneutrinosandthetopmassfrommeasurementofrsigmawellnusigmazellell
AT stubenrauchc combinedlimitsonthenumberoflightneutrinosandthetopmassfrommeasurementofrsigmawellnusigmazellell