Development of a Gamma Camera Based on an 88 Array of LaBr3(Ce) Scintillator Pixels Coupled to a 64-channel Multi-anode PMT Hidetoshi Kubo, K.Hattori,

Slides:



Advertisements
Similar presentations
GEM Chambers at BNL The detector from CERN, can be configured with up to 4 GEMs The detector for pad readout and drift studies, 2 GEM maximum.
Advertisements

1 Proton detection with the R3B calorimeter, two layer solution IEM-CSIC sept report MINISTERIO DE EDUCACIÓN Y CIENCIA CONSEJO SUPERIOR DE INVESTIGACIONES.
Advanced GAmma Tracking Array
1 Continuous Scintillator Slab with Microchannel Plate PMT for PET Heejong Kim 1, Chien-Min Kao 1, Chin-Tu Chen 1, Jean-Francois Genat 2, Fukun Tang 2,
Detection of Gamma-Rays and Energetic Particles
Towards a Compton Telescope for Gamma-Ray Astronomy in the MeV range CSNSM-Orsay, AIM/CEA-Saclay, APC-Paris, MPE-Garching, NSI-Copenhagen AHEAD meeting,
*Shuji Maeo 1,2, Takayuki Yanagida 1, Yuui Yokota 1 and Akira Yoshikawa 1,3 1 Division of Physical Process Design, Institute of Multidisciplinary Research.
Gamma Camera Technology
Tests of scintillators CsI, CsI(Na), BGO, NaI(Tl) CsI(Tl)
1 A Design of PET detector using Microchannel Plate PMT with Transmission Line Readout Heejong Kim 1, Chien-Min Kao 1, Chin-Tu Chen 1, Jean-Francois Genat.
1 SCINTILLATION LIGHT YIELD OF Ce-ACTIVATED LSO, LYSO, LuAP AND LuYAP.
Crystals and related topics J. Gerl, GSI NUSTAR Calorimeter Working Group Meeting June 17, 2005 Valencia.
GAMMA RAY SPECTROSCOPY
S. Zuberi, University of Rochester Digital Signal Processing of Scintillator Pulses Saba Zuberi, Wojtek Skulski, Frank Wolfs University of Rochester.
Lecture 2-Building a Detector George K. Parks Space Sciences Laboratory UC Berkeley, Berkeley, CA.
Copyright © Hamamatsu Photonics K.K. All Rights Reserved. Oct at NNN07 Workshop Hamamatsu Photonics Electron Tube Division Recent Progress in PMTs.
Latest developments in Hamamatsu Large Format PMTs
Report on SiPM Tests SiPM as a alternative photo detector to replace PMT. Qauntify basic characteristics Measure Energy, Timing resolution Develop simulation.
1 Performance of multi-anode PMT employing an ultra bi-alkali photo-cathode and rugged dynodes Takahiro Toizumi Tokyo Institute of Technology S. Inagwa.
Innovation is in our genes. 1 Siemens Medical Solutions Molecular Imaging What are SPECT basics?
Department of Radiology UNIVERSITY OF PENNSYLVANIA 1 Investigation of LaBr 3 Detector Timing Resolution A.Kuhn 1, S. Surti 1, K.S. Shah 2, and J.S. Karp.
Evaluation of Silicon Photomultiplier Arrays for the GlueX Barrel Calorimeter Carl Zorn Radiation Detector & Medical Imaging Group Jefferson Laboratory,
February 14, 2013 Study of a Cherenkov TOFPET modulePeter Križan, Ljubljana Samo Korpar, Rok Dolenec, Peter Križan, Rok Pestotnik, Aleš Stanovnik J. Stefan.
A novel gamma-ray detector with sub-millimeter resolutions using a monolithic MPPC array with pixelized Ce:LYSO and Ce:GGAG scintillators Takuya Kato J.Kataoka,
11 th iWoRiD, Prague, Czech Republic Low-power Wide-dynamic-range Readout System for a 64-channel Multi-anode PMT of a Scintillation Gamma Camera Satoru.
Nuclear Medicine: Planar Imaging and the Gamma Camera Katrina Cockburn Nuclear Medicine Physicist.
T. Sugitate / Hiroshima / PHX031 / Nov.01 The Photon Spectrometer for RHIC and beyond PbWO 4 Crystal Density 8.29 g/cm 3 Radiation length 0.89 cm Moliere.
MEASUREMENT Of γ-RAY ENERGY SPECTRA BY A SCINTILLATION COUNTER
Real-time Imaging of prompt gammas in proton therapy using improved Electron Tracking Compton Camera (ETCC)  TP C Pixel Scintillator Arrays (PSA) RI reagent.
A gas scintillation proportional counter for thermal neutron scattering measurements D.Raspino, N.J.Rhodes, E.M.Schooneveld (ISIS-STFC), I.Defendi, M.Jurkovic,
K. Miuchi K. Miuchi July 10, 2008 Dark Matter and Dark Energy Direction-Sensitive Dark Matter Search --NEWAGE-- Kentaro Miuchi (Kyoto University) (New.
NEWAGE Hironobu Nishimura ( Kyoto University) K. Miuchi T. Tanimori, H. Kubo, S. Kabuki, A. Takada, K. Hattori, K. Ueno, S. Kurosawa, T.Ida, S.Iwaki A.
Timing properties of MCP-PMT K.Inami (Nagoya university, Japan) - Time resolution - Lifetime - Rate dependence Photon Detector Workshop at Kobe,
Scintillator Detector and the ISIS Neutron Detector Group
Performance and applications of a  -TPC K. Miuchi a†, H. Kubo a, T. Nagayoshi a, Y. Okada a, R. Orito a, A. Takada a, A. Takeda a, T. Tanimori a, M. Ueno.
Experimental Nuclear Physics Some Recent Activities 1.Development of a detector for low-energy neutrons a. Hardware -- A Novel Design Idea b. Measure the.
R. Pani Department of Experimental Medicine and Pathology University of Rome La Sapienza-Italy. Flat Panel PMT: advances in position sensitive photodetection.
A Single Photon Emission Computer Tomograph for breast cancer imaging S. Vecchio a, N. Belcari a, P. Bennati b, M. Camarda a, R. Campanini c, M. N. Cinti.
Tracking Background GRETINA Software Working Group Meeting September 21-22, 2012, NSCL MSU I-Yang Lee Lawrence Berkeley National Laboratory.
Electron tracking Compton camera NASA/WMAP Science Team  -PIC We report on an improvement on data acquisition for a Time Projection Chamber (TPC) based.
Development of an Electron-Tracking Compton Camera using CF 4 gas at high pressure for improved detection efficiency Michiaki Takahashi N. Higashi, S.
Development of an Electron-Tracking Compton Camera with a Gaseous TPC and a Scintillation Camera for a Balloon-borne experiment (SMILE) Kazuki Ueno, Toru.
A.Ochi*, Y.Homma, T.Dohmae, H.Kanoh, T.Keika, S.Kobayashi, Y.Kojima, S.Matsuda, K.Moriya, A.Tanabe, K.Yoshida Kobe University PSD8 Glasgow1st September.
Calibration of uniformity between LYSO crystals Zhigang Wang Institute of High Energy Physics, CAS The Third International Workshop on the High.
The CALET Gamma-ray Burst Monitor (CGBM) Kazutaka Yamaoka, Atsumasa Yoshida, Yuki Nonaka, Yoko Sakauchi, Takumi Hara, Tatsuma Yamamoto (Aoyama Gakuin University),
Peter Dendooven LaBr 3 and LYSO monolithic crystals coupled to photosensor arrays for TOF-PET Physics for Health in Europe Workshop February 2-4, 2010,
A.Ochi Kobe University MPGD2009 Crete 13 June 2009.
Acquisition time6 min1 min 12 s Collimator height25 mm (Anger)12 mm (HiSens) Detector1 layer, 1 pixel / hole3 layers, 1 pixel / hole3 layers, 4 pixels.
SrCl 2 crystal for EC/  + search Presented by J.H. So (KNU)
Beam Profile Monitor for Spot-Scanning System Yoshimasa YUASA.
Room-Temperature Semiconductors: From concepts to applications Zhong He Nuclear Engineering and Radiological Sciences Department The University of Michigan,
Upgrade of the MEG liquid xenon calorimeter with VUV-light sensitive large area SiPMs Kei Ieki for the MEG-II collaboration 1 II.
A. Takada (Kyoto University)  Our motivation   -PIC and MeV gamma-ray telescope   -PIC applications  New type  -PIC.
Nucleus-Nucleus 2015, Catania,  Motivation: need for accurate ion beam range verification in hadron therapy  Method: prompt-  imaging.
CaMoO 4 at low temperature - LAAPD and PMTs - Woonku Kang, Jungil Lee, Eunju Jeon, Kyungju Ma, Yeongduk Kim Sejong University for KIMS collaboration Double.
Prostate probe with SPECT technique NSS – MIC November 5 - KnoxvilleF. Garibaldi- INFN – Roma1 – gr. Coll. ISS  the medical problem  the proposal.
12 th Pisa Meeting, Isola d’Elba, 25 May 2012 Politecnico di Milano, Italy New Development of Silicon Drift Detectors for Gamma-ray.
Presented by Samuel DUVAL On behalf of the Xénon group Industry-Academia Matching Event on Micro-Pattern Gaseous Detectors April 2012, Annecy-le-Vieux.
Hybrid Detector(s) for Complete Gamma Ray Spectroscopy S. S. Bhattacharjee, R Raut, S S Ghugre, A K Sinha UGC-DAE Consortium For Scientific Research, Kolkata.
Gamma Spectrometry beyond Chateau Crystal J. Gerl, GSI SPIRAL 2 workshop October 5, 2005 Ideas and suggestions for a calorimeter with spectroscopy capability.
from Saint Gobain studies
Development of a Compton Camera for online range monitoring
Low-power Wide-dynamic-range Readout System
On behalf of the GECAM group
A.Takada, A.Takeda, T.Tanimori
Background Reduction for Quantitative Gamma-ray Imaging with the Electron-Tracking Compton Camera in High Dose Areas May 26th, PS10A-10 T. Mizumoto,
3x3-MPPC-SMDx16ch SiPM tileable modules from Hamamatsu
First demonstration of portable Compton camera to visualize 223-Ra concentration for radionuclide therapy Kazuya Fujieda (Waseda University) J. Kataoka,
一种基于晶体间光分享原理的深度测量PET探测器
Status Report on MCP PET Simulation
Presentation transcript:

Development of a Gamma Camera Based on an 88 Array of LaBr3(Ce) Scintillator Pixels Coupled to a 64-channel Multi-anode PMT Hidetoshi Kubo, K.Hattori, S.Kabuki, S.Kurosawa, K.Miuchi, T.Nagayoshi, H.Nishimura, Y.Okada, R.Orito, A.Takada, T.Tanimori, K.Tsuchiya, K.Ueno Kyoto University, Waseda University, Kobe University, Japan IEEE 2007 NM1-1

Outline Scintillation camera in Compton camera Performance of monolithic LaBr3 Assembly of LaBr3 pixel array Performance of LaBr3 pixel array Compton camera using LaBr3 pixel array Summary

Our Compton Gamma-Ray Camera Gaseous TPC 3D track and energy of recoil electron Scintillation camera position and energy of scattered -ray 0.1a few 10 MeV g-ray  Better energy resolution of scintillator E Better angular resolution of Compton camera  (MPGD) LaBr3 (Ce) has the best energy resolution of all known scintillators. MP4-1 Tanimori, N33-5 Ueno

GSO Scintillation Camera 2006 IEEE NSS Kubo et al., GSO Scintillation Camera  64ch MAPMT(HPK Flat-panel H8500) Coupled with optical grease 88 anodes anode pitch: 6.1mm 12 stage metal channel dynode Size: 52mm52mm (Photocathode coverage ~89%) Anode uniformity: min:max~1:3 52mm Scintillation camera PSA (Pixel Scintillator Array) 66 PMTs GSO (Ce) crystal (Hitachi Chemical) no hygroscopic: it is easy to assemble radiation hard 88 pixels Pixel size: 6mm6mm13mm fits the anode-pitch of H8500 Pixels are optically isolated with the 3M ESR film (65 mm thick) 3333 cm2 2000 50mm GSO pixels

Applications of Compton camera MeV gamma-ray Astronomy Medical Imaging GSO Scintillation camera 1.4m thyroid gland phantom Balloon experiment was conducted in 2006 131I injection 364 keV M18-110 Kabuki,M13-141 Kohara, M18-150 Shirahata N59-8 Takada

LaBr3(Ce) scintillator High light yield (NaI%)160% cf.GSO(Ce)20% Fast decay time: 26 nsec hygroscopic it is difficult to assemble E.V.D. van Loef, et al., (2000) Saint-Gobain BrilLanCe380 Size:3838mm3 Energy resolution measured with a single-anode PMT(HPK R6231) FWHM(%)=(3.10.3)    (E/662keV)-0.530.02

Assembly of LaBr3 pixel array PMT package: 5252 mm2 6.1 mm pitch Area ratio: Crystal/package (5.88/54)2 =74% 54 mm 49 mm (=PMT photocathode) LaBr3 (Saint-Gobain BrilLanCe380) Size:3838mm3 54 mm 20 mm Hermetic package of aluminum(0.5mm t) Glass window(2.3mm t) We quarried two 3838 mm3 LaBr3 crystals to 5.8x5.8x15.0mm3 pixels and assembled an 88 array with a pitch of 6.1 mm (=anode pitch of H8500 PMT) by our technique. The crystal with an area of 4949 mm2 is sealed in a compact aluminum package with glass window.

Energy resolution of LaBr3 pixel array coupled to single-anode PMT To remove the effect of gain-uniformity (3) among 64 anodes of MAPMT(H8500) 2 inch square single-anode PMT (HPK R6236) Energy resolution (FWHM) of 64 pixels: 5.80.9% at 356keV 4.90.7% at 662keV collimated gamma rays were irradiated to one pixel

Readout of a 64ch Multi-anode PMT LaBr3 array 64ch MAPMT HPK Flat-panel H8500 Resistor chain board Each anode is connected to resistors, and 4 ch at the corners in resistor chains are read. X, Y positions of 64 anodes are obtained in the charge-division method. 100

Flood field irradiation image 57Co 122keV 137Cs 662keV

Light output uniformity LaBr3 8x8 pixel array Average : 71.3 RMS : 14.5 RMS/Av.=20% corrected with PMT-anode gain Maximum value is normalized to 100.

Energy spectrum of LaBr3 pixel array 133Ba 137Cs 3838mm3 monolithic crystal 22Na 8x8 pixel array

Energy resolution LaBr3 8x8 pixel array FWHM(%)=(6.20.4)    (E/662keV)-0.630.01 137Cs 662 keV worse than the 3838mm3 monolithic crystal by factor 2 88 pixel array Average 6.3% RMS 1.2% 3838mm3 crystal

GSO array vs. LaBr3 array Energy resolution GSO LaBr3 array: 6613 mm3 8x8 array: FWHM(%)=(10.40.3)    (E/662keV)-0.510.01 better by factor 1.7 LaBr3 array: FWHM(%)=(6.20.4) (E/662keV)-0.630.01

Compton camera using LaBr3 pixel array M18-110 Kabuki LaBr3 pixel array GSO Angular resolution (FWHM) [deg] 10x10x10 cm3 Gaseous TPC LaBr3 4.0deg at 662keV Improved by 2 Energy [keV] Cube phantom with 131I (364keV) 3cm with GSO array with LaBr3 array 3cm

Summary In order to improve the angular resolution of the Compton camera, we have developed an 8x8 array of LaBr3(Ce) pixels with a size of 6x6x15mm3 , sealed in a compact package, and a gamma camera based on the array coupled to a 64ch MAPMT(HPK H8500). Light output uniformity among 64 pixels is 20%(RMS). Energy resolutions (FWHM) at 662 keV are 3838mm3 monolithic: 3.10.3% 88 array with SAPMT: 4.90.7% 88 array with MAPMT by resistor-chain readout: 6.3(Av. of 64 pixels)1.2(RMS)% Angular resolutions (FWHM) of the Compton camera using the LaBr3 array are 6.1 and 4.0  at 364 keV and 662 keV, respectively. For future work, we will make four arrays to cover an area of 10x10 cm2, and develop a readout system by which each anode is read individually to improve the energy resolution.