DocumentCode :
2561745
Title :
Optimization of the in-beam OpenPET detector for carbon beam irradiation
Author :
Nishikido, Fumihiko ; Hirano, Yoshikuni ; Inadama, Naoko ; Yoshida, Erika ; Tashima, Hideaki ; Sato, Seiki ; Inaniwa, Taku ; Murayama, Hiroki ; Ito, H. ; Yamaya, Taiga
Author_Institution :
Nat. Inst. of Radiol. Sci., Chiba, Japan
fYear :
2012
fDate :
Oct. 27 2012-Nov. 3 2012
Firstpage :
3847
Lastpage :
3849
Abstract :
We are developing the OpenPET which is well suited to in-beam PET in carbon ion therapy thanks to the open space. The in-beam PET can image the distribution of positron emitters during beam irradiation for in-situ dose monitoring. Therefore careful designing and testing of OpenPET detectors are important because secondary particles generated in a target degrade detector performance in the OpenPET geometry and the quantity of positron emitters produced in in-beam PET is very small. In this paper, we optimized the final design of the in-beam OpenPET detector. Some detector components were changed from our previous work for use under practical situations. We carried out in-beam tests of this new detector for 12C beam irradiation with practical intensities. The constructed OpenPET detector consists consisted of a 16 × 16 × 4 crystal array with four-layer DOl encoding capability and a position-sensitive photomultiplier tube (PS-PMT). The scintillator material was changed from LGSO that included radio isotopes to GSOZ. In order to compensate for the lower light yield of GSOZ, we applied the PS-PMT (R10552-100-M64) with the super bialkali photocathode which realizes 30% higher quantum efficiency than the conventional bialkali type. A large current divider circuit was applied since the PMT current exceeded the dynamic range of a normal divider circuit under the targeted practical situations. Irradiation tests were done in HIMAC. The energy and intensities of the 12C beam were 290MeV/u and 1.0 × 108 particles per second (pps), respectively. The detector was positioned 30cm from the backside of the water phantom at an angle of 30deg. We obtained sufficient crystal identification performance around 1.0 × 108 pps, although the position histogram was degrading slightly with increasing 12C beam intensity. The energy resolutions of 15.2% (1st layer), 14.6% (2nd layer), 13.6% (3rd layer) and 12.- % (4th layer) were obtained for single crystal elements. We concluded that the constructed detector was able to function as the OpenPET detector for in-beam imaging.
Keywords :
biomedical equipment; carbon; ion beam effects; optimisation; phantoms; photomultipliers; positron emission tomography; radiation therapy; C; Irradiation tests; OpenPET geometry; PS-PMT; carbon beam irradiation; carbon ion therapy; conventional bialkali type; crystal identification performance; energy resolutions; high quantum efficiency; in-beam OpenPET detector; in-beam imaging; in-beam tests; in-situ dose monitoring; large current divider circuit; low light yield; open space; optimization; position-sensitive photomultiplier tube; positron emitter distribution; radioisotopes; scintillator material; secondary particles; single crystal elements; super bialkali photocathode; target degrade detector performance; water phantom;
fLanguage :
English
Publisher :
ieee
Conference_Titel :
Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC), 2012 IEEE
Conference_Location :
Anaheim, CA
ISSN :
1082-3654
Print_ISBN :
978-1-4673-2028-3
Type :
conf
DOI :
10.1109/NSSMIC.2012.6551882
Filename :
6551882
Link To Document :
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