commissioning with cosmic rays of the muon spectrometer of the atlas experiment at lhc luca spogli...
TRANSCRIPT
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Commissioning with cosmic rays of the Muon Spectrometer of the
ATLAS Experiment at LHC
Luca SpogliUniversità Roma Tre & INFN Roma Tre
LNF Frascati Spring School 2007
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Outline
The ATLAS experiment at LHC Muon Spectrometer Commisioning Status Test with cosmic rays Summary
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ATLAS detectorMuon Spectrometer
Electromagnetic Calorimeter
Solenoid
Forward Calorimeter
Endcap Toroid
Barrel Toroid
Inner DetectorHadronic Calorimeter
Radiation Shielding
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good space resolution (~100 μm per point) pt/pt 2-3% @ pt<200GeV/c
pt/pt 10% @ pt 1TeV/c
MDT (Monitored Drift Tubes)MDT (Monitored Drift Tubes)
Tubes per layer
Layer per multilayer
Chamber lenght (mm)
Chamber heigth (mm)
~~1200 chambers / 1200 chambers / ~7000 m~7000 m22
MDT RPC
TGC
CSC
ECT
=1=1.4
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MDT Calibration: r(t)
Drift time measurement Determination of space-time
relationship r(t) via autocalibration
Time measurement
rt-relation with a typical accuracy of 10µm
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Muon Reconstruction
MDT mutilayer
In a single multilayer
Track segments
Momentum measurement from sagitta determination p=0.3 Br
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Installation and commissioning
Installation in the pit started in Summer 2005
First tests with cosmic muons during Summer 2006
First curved muon (magnetic field on) in November 2006
MDT chamber installation completed in the barrel region
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Installation
It is not an easy task...It is not an easy task...
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Cosmics 19-20 November data Sector 13 with RPC timing
informations Magnetic field on-off ~1 Mevents 9 chambers Many tests on MDT’s
Drift behavior Calibration Efficiency Noise Dead channels Preliminary alignment
Some results in this talk Sector 13
Side A
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Event Display
BIL chamber
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Fired tubes per event
Accidental trigger coincidences
6 multilayers
4 multilayers
2 multilayers
Number of Fired Tubes / event
...after noise reduction cuts
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Impact of magnetic field on r(t)
B field parallel to the wire
Electrons do not travel straight forward radially
They travel under an angle ψ
Drift time t for a certain radius r increases
B field expected to change drift-to-B field expected to change drift-to-radius relationship by radius relationship by Lorentz angleLorentz angle
τ: mean time between collisions
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µ-µ+
Ratio of µ+ / µ- = 1.48±0.27
Measured muon spectra
Momentum (GeV)
According to P.D.G Charge ratio of cosmic ray muons is between 1.1 - 1.4 from 1 to 100 GeV Effects of geometrical acceptance have to be taken into account
Z coordinate
Big shaftSmall shaft
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Big shaft~18 m
Small shaft~12 m
SIDE A
SIDE C
Surface-Pit~100m
Sector 13Side A
Muons coming from the shafts, are deviated in the upper part of Muon Spectrometerbefore ending in sector 13; due to the magnetic field µ+, µ- result in different angles.
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Conclusions
Barrel installations is completed Test with cosmic muons: complete
analysis of sector 13 data Systematic study of the MDT
performance over the all barrel sectors (magnetic field off)
Further tests with cosmics in June with B field on.
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Backup slides...
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Energy per Proton 7 TeV
Bunch spacing 25 ns
Bunch size 15 m 12 cm
Protons per bunch 1011
Bunches per ring 2835
Beam mean life 10 hours
Project Luminosity 1034 cm-2 s-1
Circumference 27 Km
Collisions per bunch 25
Detection of Higgs decay final states:H ZZ 4µ “Golden Channel”
Higgs @ 114.1GeV < mH < 1 TeV
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two multilayers of 3 (in Middle and Outer two multilayers of 3 (in Middle and Outer rings) or 4 (in the Inner ring) layers of rings) or 4 (in the Inner ring) layers of staggered drift tubes each.staggered drift tubes each.
thin wall (400 μm thick) 3 cm diameter thin wall (400 μm thick) 3 cm diameter aluminum tubes.aluminum tubes.
low longitudinal diffusion gas mixture, low longitudinal diffusion gas mixture, 93%Ar−7%CO2, absolute pressure of 3 93%Ar−7%CO2, absolute pressure of 3 bar. bar.
Gold-plated W-Re anode wire, 50 μm Gold-plated W-Re anode wire, 50 μm diameter is tensioned at 350 g crimped in diameter is tensioned at 350 g crimped in copper pins.copper pins.
low gas gain of 2×10low gas gain of 2×1044 (3080 V andode (3080 V andode voltage) to avoid ageing effects.voltage) to avoid ageing effects.
good space resolution (~100 μm per point)
robust and reliable operation for many years (no ageing problems).
MDT (Monitored Drift Tubes)MDT (Monitored Drift Tubes)
From F.PetrucciFrom F.Petrucci
Tubes per layer
Layer per multilayer
Chamber lenght (mm)
Chamber heigth (mm)
~~1200 chambers / 1200 chambers / ~5500 ~5500 mm22
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Impact of resolutionImpact of resolution
Space resolution ~100 micron
Transverse momentum resolution
Z mass resolution
(combined with Inner Detector tracking)
Z->µµ
From TDR
Invariant Mass (GeV)
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ATLAS Installation Schedule 9.1
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Setup
13 Muon stations read-out
BIL
BML
BOL
BOFBOF
BIL 1BIL 3 BIL 2
BOF1BOF3
BML 3
BOL 3
Side A
From R. NikolaidouFrom R. Nikolaidou
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TDC vs ADC spectrum
Noise
Signal
AD
C c
ou
nts
TDC counts
Background
“double hits”
When a tube has a second hit in the same event.
From C.BiniFrom C.Bini
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Magnetic field map
Magnetic field strongly inhomogeneous, in particular in BILs!
From C.BiniFrom C.Bini
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Angle of tracks
µ-µ+
degrees
Angle of tracks with respect to vertical axis. Shift inspectrum for different signs (run with magnetic field on)
Muons coming from the small shaft
Big shaft
µ+ µ-
Angle of tracks: superposition of run with and without magnetic field
• µ- µ+ run with magnetic field on• µ run with no magnetic field
From R. NikolaidouFrom R. Nikolaidou