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Precision testing the Standard Model
Internal consistency of the most sensitive electroweak measurements within the standard model framework is examined. Confirming an earlier observation on the separation of Z-pole asymmetry measurements into {\em hadronisation- free}and {\em hadronisation-sensitive}, the electroweak mixing angle deri...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2001
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/516682 |
_version_ | 1780897659194703872 |
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author | Aziz, T. Gurtu, A. |
author_facet | Aziz, T. Gurtu, A. |
author_sort | Aziz, T. |
collection | CERN |
description | Internal consistency of the most sensitive electroweak measurements within the standard model framework is examined. Confirming an earlier observation on the separation of Z-pole asymmetry measurements into {\em hadronisation- free}and {\em hadronisation-sensitive}, the electroweak mixing angle derived using the former is in perfect agreement with the precision W mass. These two complimentary measurements of weak radiative corrections, when combined with the lower limit on Higgs mass, are incompatible with the measured top quark mass. To overcome this inconsistency, a scenario readily testable in Run-II at Tevatron is envisaged: an upward shift of the top quark mass by about 10 GeV ($\sim 2\sigma$). If, however, the improved top quark mass remains at its current value or the lower limit on Higgs mass moves up substantially, then abandoning the SM may become inevitable. |
id | cern-516682 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2001 |
record_format | invenio |
spelling | cern-5166822023-03-12T06:00:09Zhttp://cds.cern.ch/record/516682engAziz, T.Gurtu, A.Precision testing the Standard ModelParticle Physics - ExperimentInternal consistency of the most sensitive electroweak measurements within the standard model framework is examined. Confirming an earlier observation on the separation of Z-pole asymmetry measurements into {\em hadronisation- free}and {\em hadronisation-sensitive}, the electroweak mixing angle derived using the former is in perfect agreement with the precision W mass. These two complimentary measurements of weak radiative corrections, when combined with the lower limit on Higgs mass, are incompatible with the measured top quark mass. To overcome this inconsistency, a scenario readily testable in Run-II at Tevatron is envisaged: an upward shift of the top quark mass by about 10 GeV ($\sim 2\sigma$). If, however, the improved top quark mass remains at its current value or the lower limit on Higgs mass moves up substantially, then abandoning the SM may become inevitable.hep-ph/0110177CERN-OPEN-2001-067CERN-OPEN-2001-067oai:cds.cern.ch:5166822001-08-29 |
spellingShingle | Particle Physics - Experiment Aziz, T. Gurtu, A. Precision testing the Standard Model |
title | Precision testing the Standard Model |
title_full | Precision testing the Standard Model |
title_fullStr | Precision testing the Standard Model |
title_full_unstemmed | Precision testing the Standard Model |
title_short | Precision testing the Standard Model |
title_sort | precision testing the standard model |
topic | Particle Physics - Experiment |
url | http://cds.cern.ch/record/516682 |
work_keys_str_mv | AT azizt precisiontestingthestandardmodel AT gurtua precisiontestingthestandardmodel |