CMS tracking performance results from early LHC operation
By V. Khachatryan, A. Sirunyan, A. Tumasyan, W. Adam, T. Bergauer, M. Dragicevic, J. Erö, C. Fabjan, M. Friedl, Rudolf Frühwirth and 2,058 more. 2010
271 citations recorded by the source corpus.
The first LHC pp collisions at centre-of-mass energies of 0.9 and 2.36 TeV were recorded by the CMS detector in December 2009. The trajectories of charged particles produced in the collisions were reconstructed using the all-silicon Tracker and their momenta were measured in the 3.8 T axial magnetic field. Results from the Tracker commissioning are presented including studies of timing, efficiency, signal-to-noise, resolution, and ionization energy. Reconstructed tracks are used to benchmark the performance in terms of track and vertex resolutions, reconstruction of decays, estimation of ionization energy loss, as well as identification of photon conversions, nuclear interactions, and heavy-flavour decays.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/dd297a377de52b128c2fe9d373fcb5c28c63b7d3
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In Nuclear and High Energy Physics
- Cms Collaboration
- The Cms Collaboration
- Atlas Collaboration
- M. Raidal
- Carlo Rovelli
- Philip C. Harris
- A. Gritsan
- Nhan Tran
Citations in the corpus
- Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at sqrt(s) = 7 TeV (2011, methodology): “Second, the charge is determined from the associated trajectory reconstructed in the silicon tracker using a Kalman Filter algorithm [36].”
- Search for dark matter and large extra dimensions in monojet events in pp collisions at sqrt(s) = 7 TeV (2012, unknown): “Events are required to have at least one primary vertex [48] reconstructed within a ±24 cm window along the beam axis around the detector center, and a transverse distance from the beam axis of less than 2 cm.”
- Description and performance of track and primary-vertex reconstruction with the CMS tracker: JINST 9 (2014) 10, P10009 (2014, methodology): “Results from the commissioning of the tracker using pp collisions in 2010 are presented in [12].”
- Particle-flow reconstruction and global event description with the CMS detector (2017, unknown): “displaced vertex within the tracker volume [31, 32].”
- Measurement of jet fragmentation in PbPb and pp collisions at s NN =2.76 TeV (2014, methodology): “This procedure is based on the standard pp iterative tracking [31].”
- Observation of long-range, near-side angular correlations in proton-proton collisions at the LHC (2010, methodology): “In this analysis, the so-called CMS highPurity [22] tracks were used.”
- Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV (2017, background): “50 larger than expected [55, 56], respectively.”
- Performance of CMS muon reconstruction in pp collision events at √s = 7 TeV (2012, methodology): “Analyses involving τ leptons [45, 46] use particle-flow isolation for the muons from the τ decays, since particle flow is used for the global event reconstruction in these analyses.”