1. CMS Cathode Strip Chambers Performance with LHC Data Vladimir Palichik JINR, Dubna NEC’2013 Varna, September 10, 2013 1

2. O u t l i n e the principle of CSC working CMS muon reconstruction algorithm in the endcap cathode strip chamber spatial & time resolution with LHC data CSC local reconstruction efficiency Higgs boson with CSC data 2

3.  r  ~ 2% of strip width, i.e. ~ 100 - 120  for ME1/1 (CMS requirement: <150  ) Reconstructed hit (RecHit) in a layer is a 2-dim object representing where a hit wire(group) intersects with the hit strip position. Segment building in CSC: straight line fit to the RecHits in each of the 6 layers of one CSC. 3 View to one layer of the 6-layer CSC

4. Bremsstrahlung and e-m showering close to hard muons lead to the problems with reconstruction in the muon system 4

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6. Endcap Muon Reconstruction Endcap Muon Reconstruction Local pattern recognition: Local Regional Global (individ.detectors) (Muon system) (Muon & Tracker system) 1.Drift Tubes in the Barrel 2.CSCs in the Endcap: clusters of Digis *) fitted into RecHits, i.e. position of hits in the detector layers. 3.Track-segment building (track following & track road methods) with the compatible RecHits in muon chambers. The track-segments are selected by a goodness of fit criteria (  2 ). *) “Digis” – digitized electronic signals 6

7. Regional Muon Reconstruction Standalone Muon system (DT,CSC and RPC): I Y Station 1 Station 3 Station 2 Station 4 e.m.showers& punchthrough Multiple scattering, energy losses, bremsstrahlung, e + e - pair production etc. in Iron Yokes (I Y) Recursive track fitting (from hit to hit in endcap; with use segments in barrel) by the least squares method ( Kalman filter propagation & parameter estimation) HCALHCAL from Hadron Calorimeter (HCAL) Muon trajectory is built on a base of CSC and DT track-segments 7

8. Global Muon Reconstruction inclusion of tracker hits starts from standalone reconstructed muons, propagated through calorimeters to outer tracker surface regional track reconstruction is performed using Tracker hits within this (  )- region; to resolve the ambiguities, all the reconstructed tracks are then refitted including the tracks in the muon chambers TeV Muons: In the Tracker hard muons look like straight lines easy to reconstruct but it is impossible to estimate Pt for the straight lines. It is necessary to include hits from the Muon system into the Global reconstruction. 8

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11. 2012 resolution is similar to 2011 Pt = sqrt (Px 2 + Py 2 ) – transverse momentum 11

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13. ADC TimeBins Strips 13

14. Tag&Probe method: A global muon anywhere in the muon system (Tag) combines with a tracker-track (within CSC, Probe) and forms an invariant mass within the Z (or J/Psi) mass window. - CSC segment reconstruction efficiency is high ( >95%) both for J/Psi and Z-boson data - good agreement between data and MC 14

15. - CSC segment reconstruction efficiency is high ( >95%) - good agreement between data and MC - efficiency is uniform with Phi 15

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19. Conclusions Cathode Strip Chambers play an important role in CMS On LHC pp data: -CSC spatial resolution is about 60-150 microns per station which is in a good agreement with CMS requirements -CSC time resolution ~ 3 ns - CSC high efficiency of segment reconstruction (96-98%) 19