Precision drift chambers (MDT) for ATLAS muon system. · Chamber assembling scheme Row materials...
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Transcript of Precision drift chambers (MDT) for ATLAS muon system. · Chamber assembling scheme Row materials...
10.09.02 DESY Zeuthen 1
Precision drift chambers (MDT)
for ATLAS muon system.
G.Chelkov JINR (Dubna)
DESY Zeuthen 10 September 2002
10.09.02 DESY Zeuthen 2
SOME GENERAL INFORMATION ABOUT ATLAS MUON
SPECTROMETER.
1. The quality of the muon measurement has been one of the guiding design criteria for the ATLAS experiment.
2.. Muon spectrometer is the outer layer of ATLAS detector (average dimensions about 22 meters high and 44 meters long).
3. For the muon trajectory the determination of 3 points in the muon track are the minimum needed.
4. All together it lead us to the 5500 meters squared have to be covered by muon detectors or 400000 single drift tube detector, grouped in 1200 chambers.
10.09.02 DESY Zeuthen 3
ATLAS Detector
10.09.02 DESY Zeuthen 4
Geneva - Stockholm
10.09.02 DESY Zeuthen 5
Football ground
MDTMDT
10.09.02 DESY Zeuthen 6
HOW WE ARE CONSRUCTING OURCHAMBERS?
Given the large area of the muon spectrometer it was necessary to devise a cheap but precise means of capturing the data. Several types of coordinate detectors are used at the MUON system. I am talking now about MDT detectors only which covered the 98.6% of full area is covered by ATLAS Muon system
( 5500 from 5580m2 ).
ATLAS has opted for a system of tubes (Monitored Drift Tubes chamber or MDT-chamber) grouped in 1200 chambers.
From mentioned above it should be clear that the process of MDT chamber construction and test is naturally divided into two parts:
•Tube assembling (wiring) and test. •MDT Chamber assembling and test
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MDT Muon Chamber
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Chamber assembling scheme
Row materialsAl tubes (Menziken),end-plugs (Nief), 50μ wire (Lumo)
Clean room # I DT assembling (wiring)
•end-plug assembling•Control of Al-tubes
•DT wiring•Test of DT full length•Test of wire tension
DT QA & DC•Wire position test (X-ray)•Leak test•Complex test (Gas mixture+HV)
Row materials•In-plane align.compon
•Spacer components•Sensors (t,B)
To MPI (Munich)
Clean room #2Chamber assembling•Incoming components QC and preparation
•Spacer asssembling (gluing•In-plane alignment installat
•Gluing of tubes Layers Superlayers Camber
To CERN
10.09.02 DESY Zeuthen 9
Procedure of drift tube wiring
The incoming industrially produced components for tube wiring is:
1. Thin wall precision Al – tubes;
2. Gold plated 50 μ tungsten-rhenium wire;
3. End-plug (which consist from end-plug body with high precision reference surface, wire holder for precise wire positioning, O-rings)
But as far as the performance of MDT muon system is determined by the performance of drift tubes and moreover there is no possibility to replace/repair single detector from the muon chamber the process of tube wiring and set of the tests must be relevant (QA/QC – procedure !!).
10.09.02 DESY Zeuthen 10
Drift tube construction and tube wiring
The scheme of the tube wiring is the following:
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Drift tube components (photo)
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Wiring Line
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DT Quality Control
PDT Working parameters:
Gas mixture: Ar(93)-CO2(7) at 3 BarVoltage : 3120 V
QC requirements:Dark current at 3400 V 2nA/mMax count rate 20Hz/mMax gas leak 10-8 Bar*l/sWire tension tolerance 17gWire position tolerance 25μ
Tests Sequence:• Wire tension test ( wiring line )• Wire position test ( X-ray )• Gas leak & overpressure test• HV&Functionality test• Checking/packing/storing• Wire tension ( chamber assembling zone )
Test rate : 120 tube/day
Common solutions• Each tube have unique Id code• All tests are computer-based• All results are automatically stored in DB• Bar-code scanner is used for Id reading
10.09.02 DESY Zeuthen 14
Wire Tension Control
Simple wire tension meter based on “magnetic“ method
•Commercial PC extension board = 8 ADC & digital outputs•Custom electronic module – DC source, amplifier and
relay controlled via digital output. • Wire may by connected either to DC source (send excitation pulse) or via amplifier to ADC
• Wire excitation by current pulses• Digitization of the wire free oscillations• Oscillation spectrum extraction with FTT• Peak finding and base frequency extraction
No other equipment – even power is from PCFully programmable – easy to adopt and build-in
into any PC – based system
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Wire tension ControlAccuracy
σ = 12 mHz at 50 Hz frequency
10.09.02 DESY Zeuthen 16
Wire Tension Control
583*
5.3%31
0.3 %tubes rejected
109329130tubes tested
overallsince 1.10.2000
PDT test results
10.09.02 DESY Zeuthen 17
X-ray Test Station. Operation scheme.
Operation scheme:
Wire position tolerance : 25µ
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X-ray Test Station (CCD)
And what do we get ? –image from CCD
Reference wires completely define wire position with respect to V - groove
Accuracy σ = 2μ
10.09.02 DESY Zeuthen 19
X-ray Test Station (statistics)
PDT test results
1491.4%
720.8%
tubes rejected
107108914tubes tested
overallsince 1.10.2000
10.09.02 DESY Zeuthen 20
X-ray Test Station (photo)
10.09.02 DESY Zeuthen 21
Gas Leak Test (scheme)
Measurement principles:
Equilibrium: P=k×L P – pressureL - leak
•Use reference leak to define k !•Use He as trace gas to avoid outgasing
problem and make measurements less sensitive to system leak (no He in atmosphere)
Max leak : 10-8 bar*l/s = 0.3 mbar/day
10.09.02 DESY Zeuthen 22
Gas Leak Test (set-up)
Setup scheme:
•While first “torpedo” is under measurement another one is being prepared -“mass production”
•Measurement time ~ 3 min
Working condition in MS camera – UHV (~ 10-6 mbar)Pressure inside torpedo < 1 mbar
10.09.02 DESY Zeuthen 23
Gas Leak Test (photo)
10.09.02 DESY Zeuthen 24
Gas Leak Test (LabView)
-2.0n
-1.0n
0
1.0n
2.0n
3.0n
4.0n
5.0n
6.0n
7.0n
8.0n
9.0n
10.0n
11.0n
12.0n
00:00:00 00:01:51 00:03:43 00:05:34 00:07:26 00:09:17 00:11:09 00:13:00 00:14:52 00:16:43 00:18:35
Time (hh:mm:ss)
-2.0n
-1.0n
0
1.0n
2.0n
3.0n
4.0n
5.0n
6.0n
7.0n
8.0n
9.0n
10.0n
11.0n
12.0n
mbar
He Leak Test
LOW 6.7E-10Helium
And how do we see the result? –
Sensitivity - better then 0.5*10-9 bar*l/sAccuracy ~ 15 %
MS output for the 0.25*10-8 Bar×l/s calibration leak
0
2.0n
4.0n
6.0n
8.0n
10.0n
12.0n
14.0n
16.0n
18.0n
20.0n
22.0n
24.0n
26.0n
28.0n
30.0n
00:00:00 00:01:51 00:03:43 00:05:34 00:07:26 00:09:17 00:11:09 00:13:00 00:14:52 00:16:43 00:18:35
Time (hh:mm:ss)
0
2.0n
4.0n
6.0n
8.0n
10.0n
12.0n
14.0n
16.0n
18.0n
20.0n
22.0n
24.0n
26.0n
28.0n
30.0n
mbar
He Leak Test
LOW 1.9E-08Helium
Real graphs with trace for 2 tubes. Last one have a leak about 0.7*10-8 bar*l/s
10.09.02 DESY Zeuthen 25
Gas Leak Test (results)PDT test results
1111.1%
740.9%
tubes rejected
103958661tubes tested
overallsince 1.10.2000
10.09.02 DESY Zeuthen 26
HV & functionality test
Principles• Test a batch (up to 96) of tubes filled with
standard gas mixture for a long time• Slowly rise voltage while controlling current • Drop voltage and rise it again if necessary
for tube training•Keep low humidity in test area
Based on CAEN 546 HV power supply module:• 96 chanels , voltage is set by groups of 12• Current in each channel is controlled with 1 nA
accuracyL3 amplifier, 32-channel discriminators and
16-channel CAMAC scalers are used to control count rate
Test procedure is automaticTime consumption :
~1 hour for tube connection+ 1.5-12 hours for the test itself
Leak current limit : 2 nA/m
10.09.02 DESY Zeuthen 27
HV test (photo#1)
How it looks like:
It is possible to test up to 96 tubes simultaneously
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HV test (photo#2)
HV board
connected DTs
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HV test (results)PDT test results
490.5%
290.3%
tubes rejected
102998585tubes tested
overallsince 1.10.2000
10.09.02 DESY Zeuthen 30
QC –final results
Since 1.10.2000overall
About 2.2%
Overall
290.3%
8585490.5%
10299HV & rate
740.8%
86611111.1%
10395Gas leak
720.8%
89141491.4%
10710X-ray
310.3%
91305835.3%
10932Wire tension
RejectedTestedrejectedtestedtest
Our current results
Find us at http://nuweb.jinr.ru/~dcbp/atlas/atlas.htm
10.09.02 DESY Zeuthen 31
MDT Production and testsOur current results
Dubna Tube Production (since 01.01.2001)
0
5000
10000
15000
20000
25000
30000
35000
28.0
1.20
01
25.0
2.20
01
25.0
3.20
01
22.0
4.20
01
20.0
5.20
01
17.0
6.20
01
15.0
7.20
01
12.0
8.20
01
09.0
9.20
01
07.1
0.20
01
04.1
1.20
01
02.1
2.20
01
30.1
2.20
01
27.0
1.20
02
24.0
2.20
02
24.0
3.20
02
21.0
4.20
02
19.0
5.20
02
16.0
6.20
02
14.0
7.20
02
11.0
8.20
02
Date
Num
ber
of T
ubes
Tot
al
0
500
1000
1500
2000
2500
3000
3500
Num
ber
of T
ubes
per
Wee
k
Real/week Plan Real Plan/week
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Responsibilities and work organization.
The construction of the Muon Spectrometer is such a big effort that it is shared between many laboratories:
10.09.02 DESY Zeuthen 33
Chamber assembling (1-st ruse).
Two ruses widely used in the MDT chamber assembling procedure.
#1 - Assembling (gluing) precision components form non-very precision elements using high precision combs and glue
10.09.02 DESY Zeuthen 34
Chamber assembling (2-nd ruse).
#2 Since deformation of such large (about 10 m2) object made form Al (not from marble!) can not be eliminated, one have to be able to control (and to compensate in a reconstruction procedure!) this deformation during all time period of chamber operation.
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RASNIK
10.09.02 DESY Zeuthen 36
MDT Production. Step#1
Spacer assembling
10.09.02 DESY Zeuthen 37
MDT Production. Step#2
First layer gluing
10.09.02 DESY Zeuthen 38
MDT Production. Final stepStep#3 Turn up-side down. 2nd layer gluing
Step#4 Turn up-side down. 3d layer gluing
Step#5-7 Turn up-side down. Next layer gluing
10.09.02 DESY Zeuthen 39
Authors (not all)
35 37
31 49
31 31
25 22
10.09.02 DESY Zeuthen 40
Data collection system
10.09.02 DESY Zeuthen 41
Workshop photos