Test of an ATLAS drift tube based Level-1 muon trigger...The ATLAS Muon Spectrometer designed for...
Transcript of Test of an ATLAS drift tube based Level-1 muon trigger...The ATLAS Muon Spectrometer designed for...
Test of an ATLAS drift tube based Level-1muon trigger
Oliver Kortner, Hubert Kroha, Sebastian Nowak, Robert Richter,Sebastian Ott, Philipp Schwegler
Max-Planck-Institut für Physik, Munich
DPG-Tagung
March 25, 2014
The ATLAS Muon Spectrometer
designed for LHCnominal luminosity:
L = 1034 cm−2s−1
HL-LHC luminosity(planned, 2022):L = 7 ∗ 1034 cm−2s−1
Precision tracking chambers1150 Monitored Drift Tube Chambers (MDT)32 Cathode Strip Chambers (CSC)
Level-1 trigger chambers606 Resistive Plate Chambers (RPC)3588 Thin Gap Chambers (TGC)
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The ATLAS MDT chambers
3 or 4drift tube
layers
�
0.05 mm
W−Re wire
r
30 mm
Al tube wall
RO
HV
length: 1−6 m
width: 1 −2 m
Gas mixture: Ar/CO2 (93/7)
3 bar absolute pressure
Max. drift time: ≈ 700 ns
Single tube resolution: 80 µm
Wire positioning accuracy: ≈ 20 µm
Chamber tracking resolution: ≈ 40 µm
SupportFrame
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Performance of the existing L1 muon trigger
Total muon production cross section
pT = 20 GeV
Faketriggers
cross section forpT > 10 GeV: ∼400 nb
cross section forpT > 20 GeV: ∼47 nb
The interesting physics ismainly at pT above ∼ 20 GeV(see W,Z cross section)
The slope of the inclusive pT
spectrum is rising very steeplywith decreasing pT
−→ threshold definition of the L1trigger must be sharp to avoidhigh trigger rates from low pT
muons
ATLAS Level-1 muon trigger efficiency
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Level-1 muon trigger (HL-LHC)
50 kHz trigger rate for trigger chambersAdditional rate reduction to 20-30 kHz by use of 1 mrad precision ofthe track slope measurement by the MDT chambers at level 1
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New trigger implementation based on MDT
RPC 3 The RPC logicidentifies high-pT
candidates
The existingreadout structurewill be preserved
MDTcoord.
TowerMaster
Hit
posi
tion
inRPC3Search path
for MDT hits
MiddleCSM
InnerCSM
OuterCSM
RPC 2
RPC 1
Trigger tower (schematic)
SectorLogic
The existing L1trigger path ispreserved
CTP
Reference point for the search path
Additionalfast read-out
example barrel
Additional fast MDT read-out necessary (existing read-out takes too long)Fast read-out is triggered by RPC/TGC→ Bunch crossing ID and muon incidence angle are knownTrigger latency increases (2.5 µs to 20 µs)
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Demonstrator setup for fast MDT read-out
For first studies with real data a demonstrator setup has been designed
Properties:
Fast read-out is implemented as second TDC (40 MHz clock)→ resolution: 25√
12= 7.22 ns→ 229 µm
Fast read-out and normal read-out are used in parallel
Fast read-out data has to be analyzed offline
Fast read-out deadtime: 2500 ns
MDT chamber Standard read-outFast read-out
USB PC
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Test of new hardware and fast tracking algorithmCERN Gamma Irradiation Facility (GIF) - 2013/2014
Goal: Measurement of efficiency and resolution
Source
Cs137
500 GBq
Filters
Scintillator
Lead
Lead
Scintillator
μ (cosmic)
MDT chamber
Reference chamber
50 cm
MDT chamber used for test6 tube layers, 50 cm length
No muon beam in the GIF→ use cosmic muons
Fast read-out and normal read-out are triggered by scintillators
Angle seed according to reference chamber: 4.7 mrad
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Drift time spectra of new fast read-outData taken at CERN in 2014, no background radiation
HPTDCEntries 104564Mean 225.9RMS 191.6
Drifttime [ns]0 100 200 300 400 500 600 700 800
En
trie
s
0
50
100
150
200
250
300
350
400
HPTDCEntries 104564Mean 225.9RMS 191.6Standard read-out
Fast read-out
Spikes in fast read-out data are caused by 25 ns TDC time resolution
Data is modified with correct trigger time (spikes are smeared out)9 / 14
Resolution and efficiency of new fast read-outData taken at CERN in 2014, no background radiation
Drift radius [mm]0 2 4 6 8 10 12 14 16
Effi
cien
cy
0.8
0.82
0.84
0.86
0.88
0.9
0.92
0.94
0.96
0.98
1
Standard read-out
Fast read-out
Drift radius [mm]0 2 4 6 8 10 12 14
Res
olut
ion
[mm
]
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45
0.5
Standard read-out7.22 ns time resolutionFast read-out
Muontrack
ReferencehitsAnalysis layerAnalysishit
DResolution:
Use 5 out of 6 layers for track fitting
Calculate distance between track and hit
Correct this value with track resolution
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Fast track finding algorithm
Histogram based track pattern recognition
α
bin width
without background with background
Muons incidence angle α is used as seed
Project hits in plane perpendicular to theapproximate track and fill into histogram
Parameter:2 mm bin width of the hit histogramAt least 4 hits to set trigger
The tracks angle is finally reconstructed using linear regression
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First fast track fitting resultsShielded chamber is used as reference (seed angle resolution of 4.7 mrad)
[mrad]ref-mrecm-0.015 -0.01 -0.005 0 0.005 0.01 0.015
0
100
200
300
400
500Entries 6531
Mean -0.0001454
RMS 0.002441
85.9%
14.1%
(90.8%)
No background occupancyPattern recognition efficiency: 93.4%
[mrad]ref-mrecm-0.015 -0.01 -0.005 0 0.005 0.01 0.015
0
50
100
150
200
250
300Entries 4636
Mean -0.0002082
RMS 0.002883
80.3%
19.7%
(89.3%)
10% background occupancyPattern recognition efficiency: 74.3%
Two categories:
Good: |mrec −mref | < 3 mrad (simulated value in brackets)
Poor: |mrec −mref | ≥ 3 mrad12 / 14
Summary and Outlook
Improvement of the ATLAS muon trigger by use of MDT basedLevel-1 trigger
Demonstrator setup with additional fast MDT read-out has beendesigned
Fast read-out shows expected resolution and efficiency
Future developments
Upgrade from prototype to a production version (80 MHz clock,avoiding dead time by use of FIFO)
Implementation of fast tracking algorithm in hardware (FPGA)
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Hardware implementation
MDT_FPGA_R2
Test Setup Board
Actel FPGA
Actel FPGA
Serial configuration of ASDs
L0 Trigger Decoding
L0 Counters
L0 Counter Serial Encoding
Serial TDC data decoding
ENC (L1, ECR, EBR, GR)
Data transfer to MC
L0 Trigger Encoding
L0 Serial Decoding
ASD
ASD
ASD
HPTDC
Hit[23:0]
Serial Interface
MC USB
Windows-PC
Software
Test Setup Adaption
Analysis Extension
3 phys. trigger inputs
USB
40-pin flat cable
MDT chamber
Scintillator module
MDT L0-Trigger Prototype Scheme
Unit / Board
Chip / Circuit
Ready
To be done
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