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A Scintillator Based MuonDetector for the Linear Collider
Paul E. KarchinWayne State University
Department of Physics and Astronomy
Meeting of the Division of Particles and Fields
University of California, RiversideAugust 28, 2004
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 1 8/28/2004
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Outline
CollaborationOverview
Physics GoalsPrinciple of OperationDetector ChallengesSimulation and Pattern Recognition
Scintillatorextrusion and coating
Fibersclear-WLS splicingWLS/scintillator coupling
Photon DetectionHamamatsu MAPMT calibrationSolid State Devices: GPD, SiPMT
Resistive Plate ChambersConclusions
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 2 8/28/2004
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Scintillator Based Muon Collaboration
Fermilab: Alan Bross, H. Eugene Fisk (Co-contact Person), Kurt Krempetz, Caroline Milstene, Adam Para, Oleg Prokofiev, Ray Stefanski
Northern Illinois University: Gerald Blazey, Dhiman Chakraborty, Alexandre Dychkant, David Hedin, Arthur Maciel
Notre Dame University: Mitchell Wayne
Rice University: P. Padley, M. Matveev, J. Roberts
University of California, Davis: Mani Tripathi, Richard Breedon
University of Texas, Austin: Karol Lang
Wayne State University: Ray Brockhaus, Alfredo Gutierrez, Paul Karchin (Co-contact Person)
http://www-d0.fnal.gov/~maciel/LCD/awg_lcdmu.html
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 3 8/28/2004
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Physics Goals
•high efficiency for muons over wide momentum range
•large suppression of hadron misidentification
•improvement of calorimeter resolution for hadronic jets (“tail catcher”)
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 4 8/28/2004
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Principle of Operationmomentum from central tracking
particle ID from:
penetration of Ecal, Hcal, SC Coil, µFe
matching µ detector track with central track
Ecal & Hcal energy deposition - min. ion. vs. em or hadronic
hadronic shower tail energymeasured by analog µ detector
Tesla Detector
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 5 8/28/2004
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Detector Challengestrade-off of detector cost with physics performance
(photon yield, analog vs. digital, timing …)integration of large, expensive detector sub-system
long term stable operation of inaccessible detector
WHY IS MUON DETECTOR R&DNEEDED?
above challenges have more than one proposed solution
TECHNOLOGY IS CHANGING!
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 6 8/28/2004
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Reconstruction Algorithm Development(C. Milstene, H.E. Fisk)
see talk on Victoria Linear Collider Workshop web page
stepper algorithm takes into account effects of dE/dx and B-field
bbar event inSiD detector
start with tracker
link to muon det.
use HCAL info.
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 7 8/28/2004
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Baseline Scintillator Design
● 1 cm thick scintillator strips in slots between 10 cm thick iron plates
● wavelength shifting (WLS) fiber readout of strip
● clear fiber link between WLS fiber and photodetector
● multi-anode photomultiplier tube opto-electrical conversion
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 8 8/28/2004
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Scintillator Optionscommercially extruded scintillator with Ti02 coating
dedicated HEP extruder (NIU/Fermilab)
tyvek/VM2000 coating
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 9 8/28/2004
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Fiber Splicing R&DFNAL & Notre Dame
WLS Fiber
WLS
Fiber
Clear Fiber1.2 mm Teflon Sleeve
Joint
Thermally Fused Fiber Splice
Dual Heating Blocks Clear Fiber
Fiber – Vacuum Clamps
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 10 8/28/2004
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Splicing Test Results
1.2 mm Fiber Light Transmission 7/22/04
0500
100015002000250030003500
1 2 3 4 5 6 7 8 9 10
Fiber Number
Cou
nts
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 11 8/28/2004
1.2 mm Fiber Splice Transmission1
00.10.20.30.40.50.60.70.80.9
1 2 3 4 5 6 7 8 9 10Fiber Number
Tran
smis
sion
7/28/04
fiber from reel
light transmission of 1 m long,1.2 mm diameter, clear,straightened fiber
fiber cut and spliced
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WLS Fiber –Scintillator
Coupling Tests
1.2 mm WLS Gluing Tests
0
10
20
30
40
50
60
BC60
0 CUR
ED U
NDER
VACU
UM
RTV6
15A/
B 100
/10 C
ENTR
IFUGE
D
RTV6
15A/
B 100
/10 C
ENTR
IFUGE
D
815C
/EPIC
URE
3234
100/1
3
815C
/EPIC
URE
3234
100/1
3 CEN
TRIFU
GED
BC60
0 100
/28BC
600 1
00/28
TACK
AT E
NDS W
ITH 81
5C
TACK
AT E
NDS W
ITH 81
5C
815C
/EPIC
URE
3234
100/1
3 CEN
TRIFU
ZED
815C
/EPIC
URE
3234
100/1
3
BC60
0 PUM
PED
DOWN
BC60
0 PUM
PED
DOWN
Sample
Res
pons
e to
Cs
137
Sour
ce (n
A)
darkfarmiddlenear
Sasha Dychkant
Measurements of 1 m long strip response using a Cs137 source.
~ 15 p.e.s
May 19, 2004
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 12 8/28/2004
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Multi-Anode Photomultiplier Readout
Goals: develop electro-optical readout for scintillator/fiber prototypes calibrate single photo-electron response of MAPMT
Method: fast pulse light emitting diode with clear fiber coupling to MAPMT
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 13 8/28/2004
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Pulse Charge Distribution
1 p.e. 2 p.e.
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 14 8/28/2004
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Alternative Photon Detectors - IGeiger-mode avalanche Photo-Diodearrays (GPD)
Colorado State and aPeak (SBIR)
phase II goal: deliver 10 64-channel GPD’s with automatic quenching circuits to readout 640 WLS fibers______________________________________
Single channel solid state photodetectors can be DIRECTLY CONNECTED to the WLS fiber thus eliminating the need forclear fibers and routing of clear fiber bundles.
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 15 8/28/2004
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Alternative Photon Detectors - IISilicon Photomultiplier / Metal-Resistor-Semiconductor micro-cell (SiPM/MRS)
see Golovin and Saveliev, Nucl. Instr. Meth. A 518 (2004) 560.
1 µm by 1 µm pixels
to be used for CALICE tile-cal and NIU Tail Catcher
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 16 8/28/2004
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Resistive Plate Chamber Option
R&D Program in Italy by CaPiRe Collaboration
RPC µ detector used in BELLE
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 17 8/28/2004
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ConclusionsOptimal design of a scintillator based muon detector requires evaluation of competing hardware technologies for scintillator(extrusion method) and photon detector (MAPMT, GPD, SiPM)
A Fermilab based collaboration is developing a prototype with •TiO2 coated, extruded plastic scintillator•WLS fiber spliced to clear fiber•Hamamatsu MAPMT readout
Only US groups are working on a scintillator based muondetector, but this work currently lacks the funding needed to make a useful comparison with an RPC based detector being developed in Europe.
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 18 8/28/2004
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Supplementary Slides
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 19 8/28/2004
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Average Photo-electron yield with LED Source
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 20 8/28/2004
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Gain Measurement with LED Source
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 21 8/28/2004
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PMT Base and FE Electronics(M. Tripathi)
for 16-channelHamamatsu MAPMT
HV bias network
High speed pre-amps
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 22 8/28/2004
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TDC Readout Interface (M. Tripathi)
high speed readout of LeCroy FERA TDC system
FPGA interface to PC parallel port
ECL-LVDSBoards added
Interface toParallel Port
P. Karchin – A Scintillator Based Muon Detector for the Linear Collider page 23 8/28/2004
A Scintillator Based Muon Detector for the Linear ColliderOutlineScintillator Based Muon CollaborationReconstruction Algorithm Development(C. Milstene, H.E. Fisk)Baseline Scintillator DesignScintillator OptionsFiber Splicing R&DSplicing Test ResultsWLS Fiber – Scintillator Coupling TestsMulti-Anode Photomultiplier ReadoutPulse Charge DistributionAlternative Photon Detectors - IAlternative Photon Detectors - IIResistive Plate Chamber OptionAverage Photo-electron yield with LED Source