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Search for Second Generation Scalar Leptoquarks
This note describes a search for pair production of second generation scalar leptoquarks ($LQ$) with a final state of either two muons and two jets, or one muon, one neutrino and two jets. We use $pp$ collision data collected at $\sqrt{s}= 7$~TeV by the CMS detector, corresponding to {$2.0$~fb$^{-1}...
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1900
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Acceso en línea: | http://cds.cern.ch/record/1405702 |
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author | CMS Collaboration |
author_facet | CMS Collaboration |
author_sort | CMS Collaboration |
collection | CERN |
description | This note describes a search for pair production of second generation scalar
leptoquarks ($LQ$) with a final state of either two muons and two jets, or one muon, one neutrino and two jets.
We use $pp$ collision data collected at $\sqrt{s}= 7$~TeV by the CMS detector,
corresponding to {$2.0$~fb$^{-1}$} of integrated luminosity.
We set a 95\%~CL limit on the second generation scalar leptoquark $\sigma \times \beta^2$
or $\sigma \times 2\beta(1-\beta)$, where $\sigma$ is LQ production
cross section and $\beta$ is the branching fraction $LQ \to \mu q$. We exclude leptoquarks with masses below 632(523)~GeV for $\beta = 1(0.5)$,
where $\beta$ is the branching fraction of $LQ\rightarrow \mu\mbox{q}$. |
id | cern-1405702 |
institution | Organización Europea para la Investigación Nuclear |
publishDate | 1900 |
record_format | invenio |
spelling | cern-14057022019-09-30T06:29:59Zhttp://cds.cern.ch/record/1405702CMS CollaborationSearch for Second Generation Scalar LeptoquarksParticle Physics - ExperimentThis note describes a search for pair production of second generation scalar leptoquarks ($LQ$) with a final state of either two muons and two jets, or one muon, one neutrino and two jets. We use $pp$ collision data collected at $\sqrt{s}= 7$~TeV by the CMS detector, corresponding to {$2.0$~fb$^{-1}$} of integrated luminosity. We set a 95\%~CL limit on the second generation scalar leptoquark $\sigma \times \beta^2$ or $\sigma \times 2\beta(1-\beta)$, where $\sigma$ is LQ production cross section and $\beta$ is the branching fraction $LQ \to \mu q$. We exclude leptoquarks with masses below 632(523)~GeV for $\beta = 1(0.5)$, where $\beta$ is the branching fraction of $LQ\rightarrow \mu\mbox{q}$.CMS-PAS-EXO-11-028oai:cds.cern.ch:14057021900 |
spellingShingle | Particle Physics - Experiment CMS Collaboration Search for Second Generation Scalar Leptoquarks |
title | Search for Second Generation Scalar Leptoquarks |
title_full | Search for Second Generation Scalar Leptoquarks |
title_fullStr | Search for Second Generation Scalar Leptoquarks |
title_full_unstemmed | Search for Second Generation Scalar Leptoquarks |
title_short | Search for Second Generation Scalar Leptoquarks |
title_sort | search for second generation scalar leptoquarks |
topic | Particle Physics - Experiment |
url | http://cds.cern.ch/record/1405702 |
work_keys_str_mv | AT cmscollaboration searchforsecondgenerationscalarleptoquarks |