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The performance of the CMS Muon system with data at $\sqrt s$ = 13 TeV
The muon spectrometer of the CMS experiment is based on three different gaseous detector technologies: Drift Tube (DT) chambers in the barrel, Cathode Strip Chambers (CSC) in the endcaps, and Resistive Plate Chambers (RPC) both in the barrel and endcaps. The performance of the muon system has been s...
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| Lenguaje: | eng |
| Publicado: |
2018
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| Acceso en línea: | https://dx.doi.org/10.1063/1.5091214 http://cds.cern.ch/record/2668218 |
| _version_ | 1780962159072641024 |
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| author | Hadjiiska, Roumyana Mileva |
| author_facet | Hadjiiska, Roumyana Mileva |
| author_sort | Hadjiiska, Roumyana Mileva |
| collection | CERN |
| description | The muon spectrometer of the CMS experiment is based on three different gaseous detector technologies: Drift Tube (DT) chambers in the barrel, Cathode Strip Chambers (CSC) in the endcaps, and Resistive Plate Chambers (RPC) both in the barrel and endcaps. The performance of the muon system has been studied with LHC proton-proton collision data, collected with the CMS detector, at $\sqrt s$ = 13 TeV. The redundancy of the muon detectors ensures correct and reliable muon identification, as well as triggering, in the harsh conditions of high instantaneous luminosity. In this talk, the different components of the muon spectrometer will be described and the performance of the system will be presented in its main aspects. |
| id | cern-2668218 |
| institution | Organización Europea para la Investigación Nuclear |
| language | eng |
| publishDate | 2018 |
| record_format | invenio |
| spelling | cern-26682182022-01-14T15:04:04Zdoi:10.1063/1.5091214http://cds.cern.ch/record/2668218engHadjiiska, Roumyana MilevaThe performance of the CMS Muon system with data at $\sqrt s$ = 13 TeVThe performance of the CMS muon system during Run2Detectors and Experimental TechniquesThe muon spectrometer of the CMS experiment is based on three different gaseous detector technologies: Drift Tube (DT) chambers in the barrel, Cathode Strip Chambers (CSC) in the endcaps, and Resistive Plate Chambers (RPC) both in the barrel and endcaps. The performance of the muon system has been studied with LHC proton-proton collision data, collected with the CMS detector, at $\sqrt s$ = 13 TeV. The redundancy of the muon detectors ensures correct and reliable muon identification, as well as triggering, in the harsh conditions of high instantaneous luminosity. In this talk, the different components of the muon spectrometer will be described and the performance of the system will be presented in its main aspects.CMS-CR-2018-167oai:cds.cern.ch:26682182018-08-20 |
| spellingShingle | Detectors and Experimental Techniques Hadjiiska, Roumyana Mileva The performance of the CMS Muon system with data at $\sqrt s$ = 13 TeV |
| title | The performance of the CMS Muon system with data at $\sqrt s$ = 13 TeV |
| title_full | The performance of the CMS Muon system with data at $\sqrt s$ = 13 TeV |
| title_fullStr | The performance of the CMS Muon system with data at $\sqrt s$ = 13 TeV |
| title_full_unstemmed | The performance of the CMS Muon system with data at $\sqrt s$ = 13 TeV |
| title_short | The performance of the CMS Muon system with data at $\sqrt s$ = 13 TeV |
| title_sort | performance of the cms muon system with data at $\sqrt s$ = 13 tev |
| topic | Detectors and Experimental Techniques |
| url | https://dx.doi.org/10.1063/1.5091214 http://cds.cern.ch/record/2668218 |
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