thijs cornelissen (infn genova ) on behalf of the atlas collaboration
DESCRIPTION
Muon reconstruction performance in ATLAS. Thijs Cornelissen (INFN Genova ) On behalf of the ATLAS collaboration. Outline. The ATLAS detector Muon performance with cosmics Muon performance with collision events. The Inner Detector (or inner tracker). - PowerPoint PPT PresentationTRANSCRIPT
Physics at LHC conference 7 June 2010, T.
Cornelissen 1
Thijs Cornelissen (INFN Genova)Thijs Cornelissen (INFN Genova)
On behalf of the ATLAS collaborationOn behalf of the ATLAS collaboration
Muon Muon
reconstruction reconstruction
performance in performance in
ATLASATLAS
Physics at LHC conference 7 June 2010, T. Cornelissen
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OutlineOutline
• The ATLAS detector
• Muon performance with cosmics
• Muon performance with collision events
Physics at LHC conference 7 June 2010, T. Cornelissen
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Immersed in a solenoid field of 2 Tesla measures the trajectories of charged particles.
The ID comprises 3 sub-detectors: (resolution)Pixel : 10/115 μm in Rϕ/zSilicon strip (SCT): 17/580 μmTransition radiation tracker (TRT): 130 μm in Rϕ
The ID covers : |η| < 2.5 (2.0 for TRT) with 3 Pixel measurements, 8 SCT and ~30 TRT.
Designed for tracking efficiency >90% () and 99% () , momentum measurement with σpT /pT = 0.05% pT ⊕1% and impact parameter (at high p) = 10 m
The Inner Detector (or inner The Inner Detector (or inner tracker)tracker)
Physics at LHC conference 7 June 2010, T. Cornelissen
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The muon spectrometerThe muon spectrometer
• Immersed in a toroidal magnetic field of ~ 0.5 T (3x8 superconducting toroids)
• Precision measurement chambers and trigger chambers– MDT (Monitored Drift Tubes)– RPC (Resistive Plate Ch.)– CSC (Cathode Strip Chambers)– TGC (Thin-Gap Chambers)
• coverage |η|<2.7
Physics at LHC conference 7 June 2010, T. Cornelissen
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Muons can be reconstructed in the inner detector (ID), the calorimeters, and/or
the muon spectrometer (MS)
Several different types of reconstruction algorithms:
‘Standalone’ muons are reconstructed in the MS, then extrapolated to the vertex
‘Combined’ muons are produced by matching an ID track to a MS track, then either a
full refit or a weighted average is performed
Gives best possible momentum resolution
‘Tagged’ muons are ID tracks matched with one or more segments in the MS
Useful in particular if the momentum is insufficient to leave a full track in the MS
Initial studies focused on efficiencies and resolutions, using ~0.6 nb-1 recorded
with the minimum bias trigger
Muon reconstruction algorithmsMuon reconstruction algorithms
Physics at LHC conference 7 June 2010, T. Cornelissen
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2008 and 2009: cosmics studies2008 and 2009: cosmics studies
Physics at LHC conference 7 June 2010, T. Cornelissen
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Inner detector cosmics studiesInner detector cosmics studies
• Track parameter resolution studied by splitting cosmic track into upper and lower half, and comparing the parameters
• Tracking efficiencies very high, as expected (muons)
• Cosmics probe mainly barrel region, statistics in endcaps much lower
Physics at LHC conference 7 June 2010, T. Cornelissen
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• Momentum resolution looks promising (better than ID for pT > 100 GeV)
• Resolution studies using combined tracks ongoing
Large sectors
Small sectorsMDT residualsnarrow=98 m
Muon spectrometer cosmics Muon spectrometer cosmics studiesstudies
ATLAS preliminary
ATLAS preliminary
Physics at LHC conference 7 June 2010, T. Cornelissen
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• Most particles in the 900 GeV run had low momentum, did not make it much further than the inner tracker.
• Still, O(100) muon candidates recorded (mostly from pion/kaon decays), and even a couple of di-muon events
Muons in 900 GeV runMuons in 900 GeV run
Physics at LHC conference 7 June 2010, T. Cornelissen
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Track parameter distributionsTrack parameter distributionscombined muons
Basic track parameter distributions show good agreement between data and simulationSimulation shows contributions from prompt muons (including b/c decays) in red, early /K decays in green, late decays in white
Physics at LHC conference 7 June 2010, T. Cornelissen
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Number of ID hits on track well described by simulation (see presentation by T. Kuhl)Good agreement between data and simulation concerning number of MDT and CSC hits on track
Number of hits on trackNumber of hits on track
combined muons
2 stations
3 stations
ATLAS preliminary ATLAS preliminary
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Reconstruction efficiencies estimated by
comparing overlap between algorithms
Use tagged muons that are confirmed as
calorimeter muons, check if combined
algorithm found the muon
Efficiencies underestimated due to
contamination of sample by /K decays
Decays are often rejected by combined
algorithms
Ultimately, efficiencies will be determined
using tag&probe with resonances
First efficiency measurementsFirst efficiency measurements
ATLAS preliminary
Physics at LHC conference 7 June 2010, T. Cornelissen
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Resolution of MS tracks studied by
comparing momentum with ID
track
Expected resolution ~5% for MS
tracks, ~2.5% for ID tracks (on
average)
Asymmetric tail due to /K decays,
larger in data than in simulation
Under investigation
Momentum resolutionMomentum resolution
ATLAS preliminary
Physics at LHC conference 7 June 2010, T. Cornelissen
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Muons inside jets have much
larger energy deposits around
them
Excellent data/MC agreement
concerning energy deposits
Simulation can thus be used to
optimize isolation cuts
Muon energy deposit and isolationMuon energy deposit and isolationTra
ck
isola
tion
Calo
rim
ete
r is
ola
tion
ATLAS preliminary
ATLAS preliminary
ATLAS preliminary
Physics at LHC conference 7 June 2010, T. Cornelissen
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• First 0.6 nb-1 has been used to assess the performance of the ATLAS muon reconstruction
• Relative efficiency measurements, muon isolation studies show very good data/MC agreement
• Now working towards full program using J/s and Zs
ConclusionsConclusions
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Backup
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Composition in MC truthComposition in MC truth
ATLAS preliminary
Physics at LHC conference 7 June 2010, T. Cornelissen
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7/4/2010
State of ATLAS for first 7 TeV State of ATLAS for first 7 TeV collisionscollisions
Muon EE chambers (||~1.2) not yet installed