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Compton imaging with the PorGamRays Detector D S Judson Imaging 2010, Stockholm, 8 th -11 th June 2010.

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Presentation on theme: "Compton imaging with the PorGamRays Detector D S Judson Imaging 2010, Stockholm, 8 th -11 th June 2010."— Presentation transcript:

1 Compton imaging with the PorGamRays Detector D S Judson Imaging 2010, Stockholm, 8 th -11 th June 2010

2 Outline PorGamRays project outline Detector description Spectroscopic performance GEANT simulations Experimental Compton imaging performance Summary

3 PorGamRays: Aims Portable Gamma-Ray Spectrometer The project aims to develop a gamma-ray spectrometer that is Handheld and battery operated Able to work at room temperature Capable of providing Isotope identification Imaging Potential applications for this sensor include: decommissioning, security and safety monitoring

4 6 CZT detectors Modular design Energy range: 60 – 2000 keV PorGamRays: Schematic gamma Pixelated CZT ASIC Daughter board Motherboard Laptop

5 PorGamRays: CZT detectors Dimensions of 20 x 20 x 2 mm Pixelated (10 x 10) 2 x 2 x 2 mm voxels

6 PorGamRays: CZT detectors Dimensions of 20 x 20 x 2 mm Pixelated (10 x 10) 2 x 2 x 2 mm voxels Detector wire bonded to daughter board Data read out through custom built ASICs

7 The PorGamRays demonstrator Two CZT detectors 5 mm separation Running from external power supplies NUCAM II ASICS [1] Energy range of up to 350 keV [1] P Seller et. al., IEEE Nuclear Symposium Conf. Rec., V6, 3786, ‘06

8 Spectroscopic performance of CZT At 60 keV ( 241 Am), FWHM ~ 6 keV, noise ~ 20 keV

9 Geant4 simulations Simulated data used to evaluated the effects of the 20 keV noise level and 350 keV energy limit Simulated two CZT detectors in PorGamRays configuration Two different gamma-ray energies were used: 121 and 356 keV

10 Geant4 simulations 121 keV γ -rays deposit little energy in the scatter detector Scatterer Absorber Eγ (keV) 0 20 40 60 80 100 120 140 160 180 200 Eγ (keV)

11 Geant4 simulations 356 keV γ -rays deposit 140-220 keV in each detector Scatterer Absorber 0 50 100 150 200 250 300 350 400 Eγ (keV)

12 Source located at x = y = 100 mm z = 40 mm x (mm) y (mm) FWHM ~ 20 mm 120 100 y (mm) x (mm) Compton images – 133 Ba – 356 keV

13 x (mm) y (mm) FWHM ~ 20 mm Source located at x = 105mm y = 115 mm z = 40 mm 120 100 y (mm) x (mm)

14 Possible to resolve changes in source position of only a few mms x position (mm) x = 95 mm x = 115 mm Compton images – 133 Ba – 356 keV

15 Multi-spectral imaging 133 Ba (356 keV) 57 Co (121 keV) x = 110, y = 120 mmx = 130 mm, y =85 mm

16 Conclusions A CZT based Compton camera has been developed Energy resolution of ~ 10 % at 60 keV Position resolution of ~ 20 mm FWHM has been demonstrated Changes in position of ~ 10 mm can easily be resolved Simultaneous measurement of 2 different source demonstrated

17 Collaborators A J Boston 1, P J Coleman-Smith 2, D M Cullen 3, A Hardie 4, L J Harkness 1, L L Jones 4, M Jones 1, I Lazarus 2, P J Nolan 1, V Pucknell 2, S V Rigby 1, D P Scraggs 1, P Seller 4, J Simpson 2, M Slee 1, A Sweeney 1 and the PorGamRays collaboration. 1 The University of Liverpool 2 STFC Daresbury Laboratory 3 The University of Manchester 4 STFC Rutherford Appleton Laboratory

18 Funded jointly by the EPSRC and TSB


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