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Performance of the CMS electromagnetic calorimeter in pp collisions at √s=13 TeV

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dc.contributor.author CMS Collaboration en_US
dc.contributor.author Hayrapetyan, A. en_US
dc.contributor.author ALPANA, A. en_US
dc.contributor.author DUBE, SOURABH en_US
dc.contributor.author KANSAL, B. en_US
dc.contributor.author LAHA, A. en_US
dc.contributor.author RASTOGI, A. en_US
dc.contributor.author SHARMA, SEEMA et al. en_US
dc.date.accessioned 2025-01-31T06:28:15Z
dc.date.available 2025-01-31T06:28:15Z
dc.date.issued 2024-09 en_US
dc.identifier.citation Journal of Instrumentation, 19(09). en_US
dc.identifier.issn 1748-0221 en_US
dc.identifier.uri https://doi.org/10.1088/1748-0221/19/09/P09004 en_US
dc.identifier.uri http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/9283
dc.description.abstract The operation and performance of the Compact Muon Solenoid (CMS) electromagnetic calorimeter (ECAL) are presented, based on data collected in pp collisions at √s =13 TeV at the CERN LHC, in the years from 2015 to 2018 (LHC Run 2), corresponding to an integrated luminosity of 151 fb-1. The CMS ECAL is a scintillating lead-tungstate crystal calorimeter, with a silicon strip preshower detector in the forward region that provides precise measurements of the energy and the time-of-arrival of electrons and photons. The successful operation of the ECAL is crucial for a broad range of physics goals, ranging from observing the Higgs boson and measuring its properties, to other standard model measurements and searches for new phenomena. Precise calibration, alignment, and monitoring of the ECAL response are important ingredients to achieve these goals. To face the challenges posed by the higher luminosity, which characterized the operation of the LHC in Run 2, the procedures established during the 2011–2012 run of the LHC have been revisited and new methods have been developed for the energy measurement and for the ECAL calibration. The energy resolution of the calorimeter, for electrons from Z boson decays reaching the ECAL without significant loss of energy by bremsstrahlung, was better than 1.8%, 3.0%, and 4.5% in the |η| intervals [0.0,0.8], [0.8,1.5], [1.5, 2.5], respectively. This resulting performance is similar to that achieved during Run 1 in 2011–2012, in spite of the more severe running conditions. en_US
dc.language.iso en en_US
dc.publisher IOP Publishing Ltd en_US
dc.subject Gamma detectors (scintillators, CZT, HPGe, HgI etc) en_US
dc.subject Large detector systems for particle and astroparticle physics en_US
dc.subject Physics, Particles & Fields en_US
dc.subject 2024 en_US
dc.title Performance of the CMS electromagnetic calorimeter in pp collisions at √s=13 TeV en_US
dc.type Article en_US
dc.contributor.department Dept. of Physics en_US
dc.identifier.sourcetitle Journal of Instrumentation en_US
dc.publication.originofpublisher Foreign en_US


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