Upload
silver
View
32
Download
0
Embed Size (px)
DESCRIPTION
System Test of the ATLAS Muon Spectrometer in the H8 Beam at the CERN SPS. Erez Etzion (Tel Aviv University) , Stefano Rosati (CERN). On behalf of the ATLAS H8 Muon Test Beam Community. IEEE, 2004 Nuclear Science Symposium Rome, Italy, October 17 2004. To trigger on MUON’s, one needs: - PowerPoint PPT Presentation
Citation preview
ATLAS Muon test beam, E. Etzion, NSS 2004
1
System Test of the ATLAS Muon Spectrometer in the H8 Beam at
the CERN SPSErez Etzion (Tel Aviv University), Stefano Rosati (CERN)
On behalf of the ATLAS H8 Muon Test Beam Community
IEEE, 2004 Nuclear Science SymposiumRome, Italy, October 17 2004
ATLAS Muon test beam, E. Etzion, NSS 2004
2
MUON Spectrometer• To trigger on MUON’s, one
needs:– Fast detectors to provide moderate
Pt measurement and Bunch ID.– Azimuthal coordinate measurement
for both, MUON tracking and correct the main tracking detectors.
• To track MUON’s with a precision similar or better than the ID, one needs:– Precision detectors, with
deformations that can be followed
– Precise magnetic field mapping
– Alignment system over large distances, (relative position of chambers 30-40 microns.)
ATLAS Muon test beam, E. Etzion, NSS 2004
3
Monitored Drift Tubes
The MDT chambers are made of two multilayers of pressurized aluminium drift tubes separated by
50 to 320mm high spacer and support structure .
A multilayer consist of three (or four) layers of dense-packed drift tubes.
Each tube determines the vertical distance between a charged particle track and the wire from the arrival time of the first ionization electron.
Tubes: -outer diameter :30mm, wall thickness: 0.4mm; Wire:50m(gold-plated)-370.000 channelsGas: -Ar:N2:CH4 -mixture (91:4:5) - pressure:3 bar(absolute)HV:3.25 kV
ATLAS Muon test beam, E. Etzion, NSS 2004
4
Cathode Strip ChambersMultiwire proportional chambers determine muon position by interpolating the charge on 3 to 5 adjacent strips
Precision (x-) strip pitch ~ 5mm
Measure Q1, Q2, Q3… with 150:1 SNR to get x ~ 60 m.
Second set of y-strips measure transverse coordinate to ~ 1 cm.
Position accuracy unaffected by gas gain or drift time variations.
Accurate intercalibration of adjacent channels essential.
S = d = 2.54 mm
W = 5.6 mm
32 four-layer chambers
2.0 < || < 2.7
|Z| ~ 7m, 1 < r < 2 m
4 gas gaps per chamber
31,000 channels
Gas Ar:CO2:CF4 (30:50:20)
High voltage :3.2 kV
32 four-layer chambers
2.0 < || < 2.7
|Z| ~ 7m, 1 < r < 2 m
4 gas gaps per chamber
31,000 channels
Gas Ar:CO2:CF4 (30:50:20)
High voltage :3.2 kV
ATLAS Muon test beam, E. Etzion, NSS 2004
5
Trigger Chambers
• The first level muon trigger is derived from three trigger stations formed of Resistive Plate Chambers (very fast detectors with moderate rate capabilities) in the barrel and Thin Gap Chambers (moderately fast detectors with high rate capabilities) in the end-caps.
• Each station is made of 2(or 3) planes of strips (or wires) with x or y readout .• The trigger is based on a coincidence between a strip (or wire) hit in the 1st
station and a range of strips (or wires) in the 2nd or 3nd station. Typical momentum
resolution is 20%. • Low pt trigger: p>6GeV.• High pt trigger: p>20GeV.
ATLAS Muon test beam, E. Etzion, NSS 2004
6
Resistive Plate Chambers• Resistive Plate Chambers are gaseous,
self-quenching parallel-plate detectors.• They are built from a pair of electrically
transparent bakelite plates separated by small spacers.
Signal are induced capacitively on external readout strips.
- 420.000 channels in 596 double gap chambers.Gas: C2H2F4:isoC4H10 (97:3).HV : 9kV.Performance:-efficiency:>99%.-space-time resolution of 1cm1ns.-rate capability:~1kHz/cm².
- 420.000 channels in 596 double gap chambers.Gas: C2H2F4:isoC4H10 (97:3).HV : 9kV.Performance:-efficiency:>99%.-space-time resolution of 1cm1ns.-rate capability:~1kHz/cm².
ATLAS Muon test beam, E. Etzion, NSS 2004
7
Thin Gap Chambers
wires
strips
supports
-e+ion
ATLAS Muon test beam, E. Etzion, NSS 2004
8
Muon Test Beam setup
BIL on rotating support CSC
Magnet
BOS
MBPL
TGCs
Barrel
Endcap
ATLAS Muon test beam, E. Etzion, NSS 2004
9
Barrel Stand
• 6 barrel MDT chambers (precision tracking) Fully instrumented with FE electronics, readout with 1 MROD Fully equipped with alignment system
• 6 RPC doublets (4 BML and 2 BOL) (LVL1 trigger + tracking) 1 Trigger PAD Being upgraded now to 2 PADS ( LowPt & HighPt)
• The setup is reproducing at full scale one ATLAS barrel sector with 6 MDT+RPC stations
• 2 additional barrel MDT chambers 1 BIL on rotating support for calibration studies 1 BOS station (MDT+RPC) upstream of muon wall for noise
studies and CTB
ATLAS Muon test beam, E. Etzion, NSS 2004
10
BML
BOL
BIL - Rotating
ATLAS Muon test beam, E. Etzion, NSS 2004
11
Endcap Stand
• 11 MDT chambers (2 EI, 2EM, 2 EO) Fully instrumented with FE electronics, readout with 1 MROD Equipped with the complete alignment system (calibrated
sensors for absolute alignment) Reproducing at full scale a muon spectrometer endcap sector
• 3 TGC chambers (2 doublets, 1 triplet) Fully instrumented with on-chamber electronics
• CSC: 1 chamber being installed during last week, should be integrated soon in the combined data taking
ATLAS Muon test beam, E. Etzion, NSS 2004
12
TGC
DoubletsTGC
Triplet
ATLAS Muon test beam, E. Etzion, NSS 2004
13
Data collected until now
• A large sample of data has been collected since June• Main tests performed on detectors:
MDT LV tests in the ATLAS configuration (2 chambers/LV channel) Barrel alignment: large chambers rotations up to 8 mrad Endcap alignment: checks of sensors absolute calibration DCS – sensors, controls Noise and efficiency studies on a large scale (~1% of ATLAS) MDT-RPC cross talk studies MDT threshold scans RPC threshold and HV scans LVL1 trigger validation with TGC during the 25 ns run in June Muon system commissioning and integration
• Triggering during the muon standalone period with 10x10 or 60x100 cm2 scintillators. Self-triggering with TGC or RPC during 25ns period
• Muon detectors are integrated in the Combined Test Beam data taking since mid of August
ATLAS Muon test beam, E. Etzion, NSS 2004
14
Online monitoring
Channel vs Layer: Fast detection of Inefficiency and Noise
Channel vs Layer: Fast detection of Inefficiency and Noise
• Monitoring framework (GNAM) co-developedwith the ATLAS Tile Calorimeter Data sampling at anylevel, Allow user libraries (decoding and histograms filling) Histograms published in the interactive presenter
• Monitoring in ATHENA
Early studies algs and collected Monitor of Event Filter performance
Online presenter (for both GNAM and EF-ATHENA)
ATLAS Muon test beam, E. Etzion, NSS 2004
15
Conditions DB
CondDB
DCS Temperature LV, B field Gas, CSM params
Global Alignment
AlignmentEnd cap,
barrel
Run Parametersfrom DAQ IS
ATHENA
AMI
Plot, Monitor
PVSS interface to MySQL
runs online and offlineJTAG
•Use MySQL with dedicated interface software (MDT) or direct SQL (TGC) •Nearly a complete loop of applications using the conditions data has been implemented • All quantities needed are stored and read• MDT - High rate access for raw alignment image results (~2 sec)•TGC – Tested configuration via online and via DCS. Root, direct web access.•Access from ATHENA analysis enviroenment under development.
ATLAS Muon test beam, E. Etzion, NSS 2004
16
Offline Software• The ATHENA framework is used as offline monitoring, reconstruction and analysis tool
Exploit the test beam data as test for the ATLAS software• ByteStream converters: access to the raw data for all muon technologies (MDT, RPC, TGC,
CSC, MUCTPI): same scheme as for ATLAS Preparing data using ATLAS Muon Event Data Model for: LVL2 (MuFast) , EF (TrigMoore) , offline (MOORE, Muonboy) algorithms
• Detector Description: same as for ATLAS (MuonGeoModel) Initialization from AMDB database primary numbers in NOVA DB, special AMDB version
implemented for the CTB Using same DD for simulation and reconstruction (as in DC2)
• Offline algs (MOORE, Muonboy) as for DC and physics data• Ntuples are produced with ATHENA for offline monitoring
Useful tool for offline monitoring of detector performance Check events correlation among subdetectors Included in the Combined Ntuples Correlation Muon track InDet track
ATLAS Muon test beam, E. Etzion, NSS 2004
17
RPC preliminary results• RPC efficiency can be evaluated comparing MDT segments extrapolation with the position of RPC clusters•Tested cluster sizes and efficiecy for different HV and thresholds•Tested correlation between MDT and RPC
Efficiency vsHV and threshold
Correlation MDT-RPC
ATLAS Muon test beam, E. Etzion, NSS 2004
18
TGC preliminary results• TGC taking data during run with 25ns-bunched beam in June• Validation of the design of the Endcap muon LVL1 trigger• LVL1 trigger signal provided to the MUCTPI
– Sector logic output and MUCTPI match perfectly• DCS – operation and control • Integration with the TGC conditions database• Results on LVL1 trigger performance:
– Low-Pt efficiency 99.4%– High-Pt efficiency 98.1%
Correlation with MDT tracks
ATLAS Muon test beam, E. Etzion, NSS 2004
19
Beam momentum measurement
Momentum
GeV
Mean=108 GeVSigma=4 GeV
Magnet OFF
Magnet ON
• Exploit the bending in MBPL magnet upstream of barrel stand• Reconstruction with MOORE• Compare track angles in BILupstream of MBPL and full barrel
•P=0.3BL/•BL=3.54 Tm
ATLAS Muon test beam, E. Etzion, NSS 2004
20
Beam momentum measurement
• Sigma – not tracking res. depends on collimators settings
• Energy loss due to material upstream of the muon area: calorimeters+3.2 m of iron (muon wall)
Preliminary – MDT threshold 40 mV
Sagitta
Outer
Middle
Sagitta definition at the TB:
• Create r-z (MDT+RPC) and phi segments (only RPC),
perform pattern recognition
• Segments fit on each station
• Combination of inner and outer,compare with middle station
• Misalignment affects mean value and width
• Multiple scattering affects width
Nominal P(GeV)
Measured P (GeV)
Sigma
(GeV)
Sagitta
resolution
(m)
100 88.8 4.34 102
120 108.2 4.06 94
150 135.0 6.84 78
180 166.3 8.83 73
220 206.1 12.11 66
250 230.0 15.11 62
ATLAS Muon test beam, E. Etzion, NSS 2004
21
Comparisons with G4 simulation• Real data/G4 sim reconstruction comparison provides important feedback to the G4 validation effort •First tests: generate muons in the CTB setup (only muon detectors activated for now) at beam energies measured in data• Reconstruction with MOORE• Compare fit residuals and sagitta resolution
Data=61m
G4 =57 m
MDT fit residuals
DataG4
Athena 8.8.0
Sagitta width
ATLAS Muon test beam, E. Etzion, NSS 2004
22
Results on alignment corrections• Tests of the relative alignment system: perform chambers controlled movements and correct using the information from the optical alignment system – many tests successfully performed during 2003 test beam• Results shown here are from barrel controlled movements performed during 2004 data taking (rotations about X axis – beam axis)• Reconstruction with Muonboy in ATHENA
Rotations at the limit of the dynamical range of the alignment system(~8 mrad)
Absolute alignment is being validated (sensors calibrations)Similar studies ongoing for the endcap system
ATLAS Muon test beam, E. Etzion, NSS 2004
23
Conclusions• The muon test beam has profited of many years of tests and
experience of the muon group in H8• Many aspects of detectors integration and combined data taking
have been tested• Data taking is going on since June, Shown here:
Detector and trigger performance Detector operation and control Use of the offline software framework (ATHENA) Reconstruction algs. studies Comparisons of G4 simulation with real data Alignment
• Further studies: Another run with 25 ns bunched beam (2 weeks ago) RPC and TGC LVL1 trigger
Complete the integration of the muon trigger slice (LVL1-LVL2-Event Filter)
Alignment of the muon system Combined data taking Combined alignment, reconstruction and physics studies
Thank you