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dc.contributor.authorApyan, Aram
dc.contributor.authorBarbieri, Richard Alexander
dc.contributor.authorBaty, Austin Alan
dc.contributor.authorBierwagen, Katharina
dc.contributor.authorBrandt, Stephanie Akemi
dc.contributor.authorBusza, Wit
dc.contributor.authorCali, Ivan Amos
dc.contributor.authorDemiragli, Zeynep
dc.contributor.authorDi Matteo, Leonardo
dc.contributor.authorGomez-Ceballos, Guillelmo
dc.contributor.authorGoncharov, Maxim
dc.contributor.authorGulhan, Doga Can
dc.contributor.authorIiyama, Yutaro
dc.contributor.authorInnocenti, Gian Michele
dc.contributor.authorKlute, Markus
dc.contributor.authorKovalskyi, Dmytro
dc.contributor.authorLai, Y. S.
dc.contributor.authorLee, Y.-J.
dc.contributor.authorLevin, A.
dc.contributor.authorLuckey Jr, P David
dc.contributor.authorMarini, Andrea Carlo
dc.contributor.authorMcGinn, Christopher Francis
dc.contributor.authorMironov, Camelia Maria
dc.contributor.authorNarayanan, Sruthi A.
dc.contributor.authorNiu, Xinmei
dc.contributor.authorPaus, Christoph M. E.
dc.contributor.authorRalph, Duncan Kelley
dc.contributor.authorRoland, Christof E
dc.contributor.authorRoland, Gunther M
dc.contributor.authorSalfeld-Nebgen, Jakob Maxillian Henry
dc.contributor.authorStephans, George S. F.
dc.contributor.authorSumorok, Konstanty C
dc.contributor.authorVarma, Mukund Madhav
dc.contributor.authorVelicanu, Dragos Alexandru
dc.contributor.authorVeverka, Jan
dc.contributor.authorWang, J.
dc.contributor.authorWang, T.W.
dc.contributor.authorWyslouch, Boleslaw
dc.contributor.authorYang, M.
dc.contributor.authorWyslouch, Victoria
dc.contributor.authorCMS Collaboration
dc.date.accessioned2019-07-25T18:12:58Z
dc.date.available2019-07-25T18:12:58Z
dc.date.issued2017-01
dc.date.submitted2016-09
dc.identifier.issn1748-0221
dc.identifier.urihttps://hdl.handle.net/1721.1/121942
dc.description.abstractThis paper describes the CMS trigger system and its performance during Run 1 of the LHC. The trigger system consists of two levels designed to select events of potential physics interest from a GHz (MHz) interaction rate of proton-proton (heavy ion) collisions. The first level of the trigger is implemented in hardware, and selects events containing detector signals consistent with an electron, photon, muon, τ lepton, jet, or missing transverse energy. A programmable menu of up to 128 object-based algorithms is used to select events for subsequent processing. The trigger thresholds are adjusted to the LHC instantaneous luminosity during data taking in order to restrict the output rate to 100 kHz, the upper limit imposed by the CMS readout electronics. The second level, implemented in software, further refines the purity of the output stream, selecting an average rate of 400 Hz for offline event storage. The objectives, strategy and performance of the trigger system during the LHC Run 1 are described.en_US
dc.language.isoen
dc.publisherIOP Publishingen_US
dc.relation.isversionofhttp://dx.doi.org/10.1088/1748-0221/12/01/P01020en_US
dc.rightsCreative Commons Attribution 3.0 unported licenseen_US
dc.rights.urihttps://creativecommons.org/licenses/by/3.0/en_US
dc.sourceIOP Publishingen_US
dc.titleThe CMS trigger systemen_US
dc.typeArticleen_US
dc.identifier.citationKhachatryan, V. et al. "The CMS trigger system." Journal of Instrumentation 12 (January 2017): P01020 © CERN 2017 for the benefit of the CMS collaborationen_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physicsen_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Nuclear Science and Engineeringen_US
dc.contributor.departmentMassachusetts Institute of Technology. Laboratory for Nuclear Scienceen_US
dc.relation.journalJournal of Instrumentationen_US
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2019-06-04T12:35:39Z
dspace.date.submission2019-06-04T12:35:41Z
mit.journal.volume12en_US


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