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Development of a Compton gamma-ray camera with LaBr 3 (Ce) - PowerPoint PPT Presentation

Development of a Compton gamma-ray camera with LaBr 3 (Ce) pixellated arrays for medical imaging Shunsuke KUROSAWA K. Hattori, C. Ida, S. Iwaki, N. Higashi, S. Kabuki, H. Kubo, K. Miuchi, K. Nakamura, H. Nishimura, J. Parker, T. Sawano,


  1. Development of a Compton gamma-ray camera with LaBr 3 (Ce) pixellated arrays for medical imaging Shunsuke KUROSAWA K. Hattori, C. Ida, S. Iwaki, N. Higashi, S. Kabuki, H. Kubo, K. Miuchi, K. Nakamura, H. Nishimura, J. Parker, T. Sawano, A. Takada A , M. Takahashi, T. Tanimori, K. Taniue, K. Ueno, Y. Yanagida B Dept. of Physics, Graduate school of Science, Kyoto University, Kyoto, Japan A ISAS / JAXA, Kanagawa, Japan B World Engineering System, Kyoto, Japan SCINT2009 June 8, 2009 @ Lotte Hotel Jeju, Jeju, Korea

  2. Contents • Introduction – Electron Tracking Compton Camera (ETCC) for Medical imaging • LaBr 3 (Ce) array – Assembly of LaBr 3 (Ce) – Measurement of a LaBr 3 (Ce) array • ETCC with LaBr 3 (Ce) arrays – Setup – Imaging with the camera • Summary

  3. Medical imaging (functional image) � New radioactive tracer with new radioisotopes PET : E = 511keV It is possible that SPECT : E < 360keV we obtain various images: anti-body, enzyme, Narrow protein reaction � Multi-radioisotope Imaging With wide energy range Wide dynamic Simultaneous observation of some energy range metabolisms and interactions 139 Ce 133 Ba 131 I 198 Au 22 Na 18 F 54 Mn 65 Zn 60 Co E 167 354 364 412 511 511 835 1116 1173 [keV] 1275 1333 PET SPECT

  4. Electron Tracking Compton Camera gaseous TPC (time projection chamber) : [containing μ -PIC(MPGD), TPC GEM (Inutsuka et al. , Sauli) ] α 10cm --- energy and 3-D track of Compton-recoil electron Scintillation camera : [Pixel array Scintillator] --- energy and position of μ -PIC Event 1 ⇒ 100 scattered gamma ray Event 50 Event 10 Event 5 Event 3 Event 1 Event 2 Scintillator GEM � Large FOV (~3str) Reconstruct incident � Kinematical background rejection gamma ray event by event by comparison of two α angles Energy dynamic range: from 0.1 to ~1 MeV

  5. To obtain a higher angular resolution Angular resolution of the Compton camera depends on the energy resolution of scintillator Incident γ Angular resolution (FWHM) [degree] Δ φ Angular resolution Sci. Eng. Res. Com. Angular (ARM) @662keV Res. @662keV 4.2 ° 10.5 % 3.1 ° 7% 2.3 ° 5% Scattering 2.1 ° 3% angle φ Recoil e - α Scattered γ K : energy E : energy Calculated assuming 1, no error in position of Compton point Doppler broadening (Ar) 2, energy Res. of TPC Zoglauer et al. (2003) : 30 % @ 22 keV Eng. Res. (FWHM) of LaBr 3 (Ce) : m e c 2 K ~ 3 % @ 662 keV cos φ = 1 - ( E + K ) E Loef et al . (2001)

  6. Assembly of LaBr 3 (Ce) array Using our technique, we cut 5.8 × 5.8 × 15.0mm 3 pixels out of two φ 38 × 38 mm 3 LaBr 3 crystals and assembled an 8 × 8 array. 6.1 mm pitch (=multi-anode PMT H8500 anode pitch) Saint-Gobain BrilLanCe380 Size: φ 38 × 38mm 3 54mm Eng. Res.: ~3 % (FWHM, @ 662 keV, using HPK R6231) 20mm Effective area : 49 × 49 mm 2 1/2 attenuation length (=PMT photocathode) @662keV Glass window : Quartz (t 2.3 mm) LaBr 3 (Ce): 18 mm Hermetic package : Aluminum ( t 0.5 mm )

  7. 4ch readout with multi-anode PMT � Flood field irradiation image using a Charge-division method Multi-anode PMT HPK H8500 137 Cs LaBr 3 (Ce) 54mm array 4ch readout with a resister chain 64 anodes of PMT 4 ch output pre.AMP R=100 Ω anode

  8. Energy resolution (FWHM) Using Multi-anode 133 Ba PMT H8500 (FWHM) @ 662 keV [%] Energy Resolution 8x8 pixel array (sum of all pixels) FWHM Eng. Res. @ 662 keV FWHM(%)= (5.7 ± 0.4) × (E/662keV) - 0.53 ± 0.01 Ave. ± σ : 5.8 ± 0.9%

  9. 9 arrays: Energy Resolutions (FWHM) @ 662keV 180cm 20mm-thickness Energy resolution (FWHM) @ 662 keV Eng. Res. (FWHM) @ 662 keV Ave. ± σ : 6.0 ± 1.0% (15mm-thickness) 5.6 ± 0.8% (20mm-thickness) 5.8 ± 0.9% (Total, 576 pixels) 180 cm

  10. Setup of ETCC LaBr 3 TPC source Source e - γ γ 2m 50mm 200mm FOV: 400cm 2 @10cm from TPC LaBr 3 (Ce) arrays Gaseous TPC 356keV, FWHM Reconstruction Angular resolution γ γ (FWHM) [degree] of a Compton event Electron e - 4.2 ± 0.3 ° 3-D track e - γ @662 keV γ 2mm

  11. Mouse imaging 65 Zn 2+ (1116keV) 131 I-MIBG (365keV) Imaging (ETCC & CT) Imaging (ETCC & photo)

  12. 131 I-MIBG (365keV) & 18 F-FDG (511keV) imaging The clinical drugs 18 F-FDG (PET) and 131 I-MIBG (SPECT) can image the MRMT1 (mammary tumor) and PC12 (Pheochromocytoma)

  13. Summary • we assembled an 8 × 8 LaBr 3 (Ce) pixel array. – Pixel size : 5.8 × 5.8 × 15 mm 3 5.8 × 5.8 × 20 mm 3 – Pixel pitch: 6.1mm (the same as that of the multi- anode PMT H8500) • Dynamic energy range: 80 – about 1000 keV. • Energy resolutions of the array with the MAPMT ( FWHM 、 @662keV ) . – 5.8 ± 0.9% (average of 9 arrays) • Angular resolution of ETCC ( FWHM 、 @662keV ) . – 4.2 ± 0.3 deg. • We observed mouse imaging: – High energy isotope : 65 Zn 2+ (1116keV) – 131 I-MIBG (365keV) & 18 F-FDG (511keV) Simultaneously

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