Performance of CMS muon reconstruction in pp collision events at √s = 7 TeV

By Burak Han Alver, G. Bauer, J. Bendavid, W. Busza, E. Butz, I. Cali, M. Chan, V. Dutta, G. Gomez-Ceballos, M. Goncharov and 26 more. 2012

842 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/81adbd8ab4f48dc58e0bae4e28c1ee208890d149

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Citations in the corpus

• Identification techniques for highly boosted W bosons that decay into hadrons (2014, methodology): “Two algorithms are used to reconstruct muons [24]: one proceeds from the inner tracker outwards, while the other starts from tracks measured in the muon chambers and matches them to those reconstructed in the silicon tracker.”
• Search for a Higgs boson decaying into a Z and a photon in pp collisions at $s$ = 7 and 8 TeV (2013, methodology): “Muon combined identification and isolation efficiencies of better than 95% have been maintained [4,5] after improving the pileup corrections with respect to those used in [19] for low luminosity data.”
• Measurement of the top quark mass using proton-proton data at √s=7 and 8 TeV (2016, background): “The momentum of muons is obtained from the track momentum determined in a combined fit to information from the silicon trackers and the muon detectors [34].”
• Description and performance of track and primary-vertex reconstruction with the CMS tracker: JINST 9 (2014) 10, P10009 (2014, methodology): “A “tag-and-probe” method [47, 48] allows an extraction of muon tracking efficiency directly from decays of known resonances.”
• Particle-flow reconstruction and global event description with the CMS detector (2017, methodology): “For nonisolated global muons, the tight-muon selection [35] is applied.”
• Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV (2017, background): “2, requiring exactly one isolated muon or electron with pT > 30 GeV and satisfying tight identification criteria [9, 10] and exactly four jets with pT > 30 GeV to reduce the possible number of jet-quark assignments.”
• Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s=13 TeV (2018, methodology): “The residuals between extrapolated tracker tracks and segments are studied using the tag-and-probe technique [2].”
• Measurement of angular parameters from the decay B0 → K⁎0μ+μ− in proton–proton collisions at s=8TeV (2017, methodology): “[38] CMS Collaboration, Performance of CMS muon reconstruction in pp collision events at √s = 7 TeV, J.”
• Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at s=13$$ \sqrt{s}=13 $$ TeV (2017, methodology): “4 and p T > 5 GeV are reconstructed by combining information from the silicon tracker and the muon system [27].”
• Search for a standard model Higgs boson produced in association with a top-quark pair and decaying to bottom quarks using a matrix element method (2015, background): “Muons are reconstructed from a combination of measurements in the silicon tracker and in the muon system [55].”
• Inclusive search for a vector-like T quark with charge 2/3 in pp collisions at √s=8 TeV (2014, methodology): “[26] CMS Collaboration, Performance of CMS muon reconstruction in pp collision events at √ s = 7 TeV, J.”