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Operation of the CMS Tracker at the Large Hadron Collider. ÖPG/FAKT Annual Meeting Salzburg. CMS: Compact Muon Solenoid. SiTracker (Pixel and Strips). Muon System. Magnet Return Yoke. Very Forward Calorimeter. Supraconducting Magnet (4 T). Weight: 12.500 t
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Operation of the CMS Tracker at the Large Hadron Collider Thomas Bergauer (HEPHY Vienna) ÖPG/FAKT Annual Meeting Salzburg
CMS: Compact Muon Solenoid SiTracker (Pixel and Strips) Muon System Magnet Return Yoke Very Forward Calorimeter Supraconducting Magnet (4 T) Weight: 12.500 t Diameter: 15 Length: 21.5 m Electromagnetic Calorimeter Hadronic Calorimeter Thomas Bergauer (HEPHY Vienna)
CMS Silicon Strip Tracker • Largest silicon tracker built • Active area of 198 m2 • 5.4 m long, 2.4 m diameter • Components: • Pixel detector (not covered in this talk) • TIB (Inner barrel): 4 layers • TID: 3 Inner Disks • TOB: (Outer Barrel): 6 layers • TEC (Endcaps): 9 disks on each side • Key features: • 9.6 Million readout channels • Analog readout Endcap (FPIX) L ~ 90 cm rmin = 4.4 cm rmax = 10.2 cm Barrel (BPIX) Thomas Bergauer (HEPHY Vienna)
CMS Tracker in pictures Thomas Bergauer (HEPHY Vienna)
CMS Tracker Installation December 2007 Thomas Bergauer (HEPHY Vienna)
Angular coverage down to 9 degree to the beam-pipe (|η|<2.5) • 4 layers and 3 rings contain stereo modules for 2D hit reconstruction Basic Building Block: Detector module • 15 148 pieces in total • 15 different geometries • Modules consist of • Carbon fiber/graphite frame • Front-end hybrid with APV25 readout chips • One or two p-on-n silicon sensor(s), 320/500 micron thick 9. September 2010 Thomas Bergauer (HEPHY Vienna)
Readout Chain Thomas Bergauer (HEPHY Vienna)
Commissioning Procedures • Analog readout • Digitization is done only in off-detector electronics (FEDs) • Thus, detector needs to • Time-align internally (different cable lengths) • Tune laser gain (analog opto-hybrids) • Optimize chip parameters (baseline,…) • Determine noise and pedestals (zero-suppressed data) • Benefit of analog readout • Higher position resolution • Makes debugging easy Thomas Bergauer (HEPHY Vienna)
Operational fraction of SST • 98.1% of channels in operation • TIB/TID: 96.3 % • One ring lost (short, appeared with B field), ~1% • HV missing and HV shorts, ~2.5% • TOB: 98.8 % • One ring lost (short, comes/goes with B field) • TEC: 99.0 % • One HV PG missing (short) • One LV PG missing (short) TID+ TEC+ TOB TIB TID- TEC- Thomas Bergauer (HEPHY Vienna)
Signal-to-Noise Ratios • Charge clusters of associated tracks • Divided by noise determined during calibration (pedestal) run • Non-perpendicular tracks normalized by trigonometry • Landau convoluted with Gaussian • MP value taken for summary Thomas Bergauer (HEPHY Vienna)
15148+1440 sensors 6 degree of freedom each O(10mm) accuracy Minimization hit/track residuals c2 Two approaches: Millipede (II): Global minimization “Hits and Impact Points” (HIP): local minimization of sensor position, iterative, detailed track model Kalman Filter-based fit method working on “correlated” elements, iterative Applied sequentially from large substructures to sensor level Distributions of Mean Residual (DMR): median of the residual distributions in each sensor Tracker Alignment p>3 GeV/c pT>0.65GeV/c Only modules with >200 hits • 2010 cosmics and collision events used for present alignment: • 1.5M cosmic tracks (p>4 GeV) • 1.7M collision tracks (p>3 GeV) • with constraint to primary vertex Thomas Bergauer (HEPHY Vienna)
Summary • CMS Tracker (together with whole CMS experiment) performs excellently in both cosmics and pp collision runs • 98,1 % channels in operation • Tracker uses analog readout from detector to off-detector electronics • Makes different calibration runs necessary • Signal-to-noise ratio meets expectations • Alignment algorithms reveal accuracy of 10μm • Tracker contributes to the high quality physics data CMS delivers Thomas Bergauer (HEPHY Vienna)
Thank you for your attention THE END Thomas Bergauer (HEPHY Vienna)
APV25 Peak vs. Deconvolution mode • Deconvolution mode • output charge for each strip represents a weighted sum of three consecutive pipeline cells • designed to avoid signal pile-up in high luminosity operations • necessary whenever bunch separation is less than a few hundred nanoseconds Thomas Bergauer (HEPHY Vienna)
pp Collisions Dec 2009 (900GeV+2.36 TeV): ~300k MinBias Events 2010 (7 TeV): ~3000 nb-1 Cosmics muons 2008: 3M tracks in tracker 2009: 4M tracks 2010: 2.2M tracks ~ 4% in pixel detector volume alignment, calibration, noise, resolution Collected Events Thomas Bergauer (HEPHY Vienna)
Track Reconstruction Efficency Tracks reconstructed in three steps: • seeding: hit triplets (mainly pixel hits) or pairs + beam spot used as track candidate • Pattern recognition: track candidate propagation (Kalman filter), addition of new compatible measurements, track candidate cleaning • Final Track Fit: track parameter estimator • Track Selection: fakes rejected with quality cuts Iterated several times: • hits associated to reconstructed tracks are removed • different seeding algorithms • different quality cuts Thomas Bergauer (HEPHY Vienna)
Impact parameter transverse longitudinal Thomas Bergauer (HEPHY Vienna)