AGATA Advanced Gamma Tracking Array
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Transcript of AGATA Advanced Gamma Tracking Array
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AGATAAGATAAdvanced Gamma Tracking ArrayAdvanced Gamma Tracking Array
Determination of position-dependent pulse Determination of position-dependent pulse shapes of Ge detectorsshapes of Ge detectors
N.GoelN.Goel,,T. Engert, J. Gerl, C.Domingo,T. Engert, J. Gerl, C.Domingo,
I. Kojouharov, H. Schaffner,S. TashenovI. Kojouharov, H. Schaffner,S. Tashenov
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Outline of the talkOutline of the talk
1. Introduction Fundamental parameters of -detector arrays
1. Total photopeak efficiency 2. Energy resolution -> - spectroscopy with relativistic beams
2. AGATA 1. Tracking
2. Pulse shape analysis
3. Scanner at GSI 1. Principle
2. Experimental position dependent pulse shapes
4. Limitation and improvements in first prototype
1. Tests with LYSO crystal scintillator
2. New scanning approach
5. Conclusions
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IntroductionIntroductionPhotopeak efficiency-high multiplicity Photopeak efficiency-high multiplicity -ray -ray cascadescascades
BGOshields
Ge
Suppress the Compton scattered events
30% of total solid angle covered by Ge
Adjacent Gecrystals operated in ADD BACK mode
For high multiplicity M, wrong summing of energies takes place
Discrimination between scattered events and individual hits possiblewith TRACKING
COMPOSITE DETECTORS SEGMENTED DETECTORSSHIELDED DETECTORS
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IntroductionIntroductionEnergy resolution: Energy resolution: spectroscopy with spectroscopy with relativistic beamsrelativistic beams
SegmentedDetectors
Reduced solid angle with segmentation/ ~ sin( Φ)•
∆Φ
Intrinsic resolution 2.5keV@ 1.3MeVDoppler Effect@(v/c) ~ 0.5
First interaction point hasposition resolution proportional to the size of segment
Analysis of segment pulse shapesgives position resolution even smaller than the size of segment
Φ
∆Φ
∆Φ
∆Φ
Φ
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Outline of the talkOutline of the talk
1. Introduction Fundamental parameters of -detector arrays
1. Total photopeak efficiency 2. Energy resolution -Spectroscopy with relativistic beams
2. AGATA 1. Gamma ray tracking2. Pulse shape analysis
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AGATAAGATAAAdvanced Gamma Tracking dvanced Gamma Tracking ArrayArray
4π gamma tracking array for nuclear physics experiments at European accelerators providing radioactive and highly intense stable beams
61.08mm
52.0
9m
m
60o
90 m
m
10o
0
612
24
18 713
19
311 25
814
20
2632
2
159
333
27
21 1016
22
28
344
1117
23
355 2930
10o
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AGATAAGATAGamma ray trackingGamma ray tracking
Recognize the individual 3D interaction points
Reconstruct the track of photon using Compton scattering formula
Full energy events distinguished from scattered events => improved photopeak efficiencyDetermining the incoming direction with a very good position resolution( 2-3mm)
Doppler shift in energyfor v/c ~ (0.2 -0.5)
E' = E ( 1- (v/c) cos )
Φ
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AGATAAGATAPulse Shape AnalysisPulse Shape Analysis
time(ns)time(ns)
Radial dependence of pulse shape
For each event, 37x100 samples of
preamplifier signals
Digital electronics to record the segment
signals
am
plit
ud
e(a
dc
un
its)
am
plit
ud
e(a
dc
un
its)
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Improvement in Doppler Improvement in Doppler correction with segmentation correction with segmentation and PSAand PSAIN-Beam test at Cologne, GermanyIN-Beam test at Cologne, Germany
1. The center of the detector.
2. The center of the firing segment.
3. Position given by pulse shape analysis.
48Ti(d,p)49Ti 100MeV
Det = 32 keV1382 keV Seg = 11 kevDet = 32kevPSA = 5.5 keVSeg = 11 keVDet = 32keV
Energy resolution
F. Recchia , ACTA PHYSICA POLONICA B Vol.38(2007)
∆Φ
Energy(keV)
Cou
nts
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SCANNERSCANNERPSA requires a system to scan the detectorPSA requires a system to scan the detector
For interaction at each 3D point inside a segmented detector, there corresponds a unique pulse shape.
A data base containing pulse shapesfor all possible interaction
position inside the detector
An efficient system to scan thedetector
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Outline of the TalkOutline of the Talk
1. Introduction Fundamental parameters of -detector arrays
1. Total photopeak efficiency 2. Energy resolution - Spectroscopy with relativistic beams
2. AGATA 1. Tracking
2. Pulse shape analysis
3. Scanner at GSI 1. Principle
2. Experimental position dependent pulse shapes
4. Limitation in first prototype
1. Tests with LYSO crystal scintillator
2. New Scanning approach
5. Conclusions
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SCANNER PRINCIPLESCANNER PRINCIPLEDetermination of incoming direction of photonDetermination of incoming direction of photon
22Na → 2γ, 511 keV
256x scintillatorfibres
4x 64 channel PMTs
Ge detectorto be scanned
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SCANNER PRINCIPLESCANNER PRINCIPLEDetermination of incoming direction of photonDetermination of incoming direction of photon
X = (b+c)/(a+b+c+d) Y = (a+b)/(a+b+c+d)-> A matrix is reconstructed which gives map of (X,Y).
X(arb units)
Y(a
rb u
nit
s)
a
b
d
c
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SCANNER PRINCIPLESCANNER PRINCIPLEDetermination of Z coordinate of interaction positionDetermination of Z coordinate of interaction position
22Na → 2γ, 511 keV
256x scintillatorfibres
6 ring slits
42 BGOs
4x 64 channel PMTs
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False Event
SCANNER PRINCIPLESCANNER PRINCIPLEEnergy spectra under triple coincidence and Agata Energy spectra under triple coincidence and Agata energy gateenergy gate
Even under triple coincidence events its possible to have false events which can be filtered by applying gate on AGATA energy.
511keV511keV
false triggering of BGO
90o scattering
True Event
Energy(keV)
Counts
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6 7 9 10 11
12
8
13 14 15 16 17
18 19 20 21 22 23
time(ns)
am
plit
ude(A
DC
unit
s)
14
SCANNERSCANNER Experimentally determined pulse shapes Experimentally determined pulse shapes
15
20 21
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SCANNERSCANNERRadial position informationRadial position information from net charge from net charge collecting segmentcollecting segment
1. Pulse rises slowly for interaction occuring close to central or outer electrode.
2. Pulse for interaction near central electrode is convex while concave for the interaction near outer electrode.
3. Pulse rises faster for interaction occurring in the middle of the segment.
1
23
1
1 2
3
time(ns)am
plit
ude(A
DC
unit
s)
time(ns)
am
plit
ude(A
DC
unit
s)
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SCANNERSCANNERRadial position information from polarity image Radial position information from polarity image chargecharge
+ve -> Interaction close to outer electrode -ve-> Interaction close to the centre electode
time(ns) time(ns)am
plit
ude(A
DC
unit
s)
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SCANNERSCANNERAzimuthal position information from amplitude of Azimuthal position information from amplitude of image chargeimage charge
Segment fired
The height of pulses from the segments close to the segment which is fired for a given event is strongly related to the point
at which the interaction tookplace.
time(ns)
am
plit
ude(A
DC
unit
s)
Pulse shapesfrom neighbouring segment
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SCANNERSCANNERSummarySummary
2 types of signalshave to be analysed
net charge signal from hit segment
Transient charge signal induced in neighbouring segment
Radial position is given by rise time and shape of pulse
Azimuthal position
Radial position
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Outline of the TalkOutline of the Talk
1. Introduction Fundamental parameters of -detector arrays
1. Total photopeak efficiency 2. Energy resolution - Spectroscopy with relativistic beams
2. AGATA 1. Tracking
2. Pulse shape analysis
3. Scanner at GSI 1. Principle
2. Experimental position dependent pulse shapes
4. Limitation and improvements in first prototype
1. Tests with LYSO crystal scintillator
2. New Scanning approach
5. Conclusions
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Limitation in the first scanner Limitation in the first scanner prototypeprototype
1. Efficiency of fibres???Most of the Compton electrons leave the active volume of fibres .Due to length of Fibre(8cm) light collection suffers.Much lower count rate contrary to expectation.
2. Low count rate problemThe true coincidence rate for back segments is about 1 count/hour.
BGO
90mm
10mm
1 ct/hr
40ct/hr
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Replacement of fibres with Replacement of fibres with LYSO/BGOLYSO/BGO
Position sensitive PMT
Scintillator plate
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Tests with LYSO crystal Tests with LYSO crystal scintillatorscintillator
-> Position resolution of LYSO plate
->Wrapping the upper surface of cyrstal for better light collection
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Tests with LYSO crystal scintillatorTests with LYSO crystal scintillator POSITION RESOLUTIONPOSITION RESOLUTION
6cm
6cm
3 mm thick
Position sensitive PMT
0.3 mm
LYSOReference detector
SETUP FOR MEASUREMENT OF POSITION RESOLUTION
7.6 cm
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Energy gate on LYSOand reference detector
to filter false events
Tests with LYSO crystal scintillatorTests with LYSO crystal scintillator Position ResolutionPosition Resolution
X
Ywidth
2.3mm
Pulse height(channel number) Pulse height(channel number)
cou
nts
cou
nts
Y(arb units)
cou
nts
511 keV 511 keV
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Tests with LYSO crystal scintillatorTests with LYSO crystal scintillator Position ResolutionPosition Resolution
74.0 74.5 75.0 75.5 76.0 76.5 77.0 77.5 78.0 78.5 79.0 79.5 80.0
0.2
0.3
0.4
0.5
0.6
0.7
0.8
Y m
easu
red
YReal
Distortion near the edges of plate.Linear central region is approximately 3cm.An accurate position calibration, allows to determine the spatial resolution (in mm). It has an average value of 2.5 mm.
surface of LYSO 0.3mm
reference detector
moved in steps of 1mm
Measured position of sourceCalc
ula
ted p
osi
tion o
f so
urc
e
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Tests with LYSO crystal scintillatorTests with LYSO crystal scintillator 2. Wrapping material for better light collection2. Wrapping material for better light collection
•Signal amplitude is higher with Enhanced Specular Reflector(ESR) film as compared to Teflon by a factor of ~ 1.32(30% light collection improvement)
•Higher reflectance increases light collection efficiency.
•Finally the upper surface of LYSO is covered with combination of Teflon and ESR.
Amplitude
TEFLON
ESR
Peak pos.= 346.591
Peak pos.= 457.365
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IImprovements possible:mprovements possible:
Circular and bigger scintillator crystals(LYSO/BGO)
Edge effects
32 anode signals of HAMAMATSU R2486
Edge effectsPosition accuracy
0.1 mm precision X-Y table Efficient and reliable measurements
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NEW SCANNING APPROACHNEW SCANNING APPROACH
X-Y detector
Ge-DetectorSide scanning detector
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Recording the pulse shapes for two positions (a) and (b).Comparing the pulse shapes from two data setsSignal of one set will be identical to signal of other set at the crossing points.
NEW SCANNING APPROACHNEW SCANNING APPROACH
Na-22 source
Na-22
Position sensitive Detector
a)
b)
90o
Rotated by 900
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Conclusions:Conclusions:
1. The next generation of arrays for in-beam -ray spectroscopy will be based on the concepts of pulse shape analysis (PSA) and - -ray tracking.
2. Using pulse shape analysis , we can get the position of first interaction point within the hit segment of a multisegmented detector.
3. Experiments have been done already to demonstrate the Doppler correction capability of AGATA detector.
4. GSI implemented a first detector scanner based on principles of PET.
5. Clear capability to obtain the scanning information was demonstrated.
6. Low efficiency of fibre detectors resulted in scanning 10 times slower than originally expected.
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Continued....Continued....
7. For this reason , we plan to replace fibres by crystal scintillators.
8. Test done with LYSO coupled to a position sensitive PMT show a position resolution of ~ 2.5 mm and an efficiency of 10% at 511 keV.
9. Pulse shape comparison procedure is proposed for measuring the HPGe detector pulse shapes as a function of the -ray interaction position inside the detector volume.
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DANKE SCHOEN
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HAMAMATSU R2486HAMAMATSU R2486
Multianode wires crossing each other in X-Y directions.
12 stage coarse mesh dynode structure.
Anode signals taken from 4 corners labelled as Xa,Xb,Ya,Y
->variables (X,Y) are calculated usingX =(Xa/Xa+Xb) Y=(Ya/Ya+Yb)
->A matrix is reconstructed which gives map of (X,Y).
POSITION POSITION RESOLUTIONRESOLUTION
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SIMULATED RESULTS OF SIMULATED RESULTS OF PERFORMANCEPERFORMANCE
CONFIG. NO.OF DETECTORS
AMT. OF GERMANIUM(Kg)
Eph[P/T]%My=1
Eph[P/T]%My=30
Ideal 4pi shell
1 233 65[85] 36[60]
AGATA 180 60 clusters 320 38[53] 24[44]
EUROBALL ~120 210 9[56] 6[37]
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Matrix ReconstructionMatrix Reconstruction
-> variables (X,Y) are calculated usingX = (b+c)/(a+b+c+d) Y = (a+b)/(a+b+c+d)-> A matrix is reconstructed which gives map of (X,Y).
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Liverpool Scanning System:Liverpool Scanning System:
Limitations in the Liverpool Scanning table: -> Uncertainities in the position determined in the X-Y direction due to finite diameter of collimator.-> Time required to scan along 9 radial lines in steps of 1 mm ~ 90 days.-> Count rate in back segments is extremely small, 1ct/ hour
34BGO's
Cs-137