A phoswich detector design for improved spatial sampling in PET

被引:5
作者
Thiessen, Jonathan D. [1 ,2 ,3 ]
Koschan, Merry A. [4 ]
Melcher, Charles L. [4 ]
Meng, Fang [4 ]
Schellenberg, Graham [5 ]
Goertzen, Andrew L. [3 ,5 ]
机构
[1] Lawson Hlth Res Inst, Imaging Program, London, ON, Canada
[2] Univ Western Ontario, Dept Med Biophys, London, ON, Canada
[3] Univ Manitoba, Dept Radiol, 702 John Buhler Res Ctr,715 McDermot Ave, Winnipeg, MB R3E 3P4, Canada
[4] Univ Tennessee, Scintillat Mat Res Ctr, Knoxville, TN USA
[5] Univ Manitoba, Dept Phys & Astron, Winnipeg, MB, Canada
基金
加拿大自然科学与工程研究理事会;
关键词
Positron emission tomography; Phoswich detector; LSO; RESOLUTION RESEARCH TOMOGRAPH; PERFORMANCE EVALUATION; ECAT HRRT; SCANNER;
D O I
10.1016/j.nima.2017.11.036
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
Block detector designs, utilizing a pixelated scintillator array coupled to a photosensor array in a light-sharing design, are commonly used for positron emission tomography (PET) imaging applications. In practice, the spatial sampling of these designs is limited by the crystal pitch, which must be large enough for individual crystals to be resolved in the detector flood image. Replacing the conventional 2D scintillator array with an array of phoswich elements, each consisting of an optically coupled side-by-side scintillator pair, may improve spatial sampling in one direction of the array without requiring resolving smaller crystal elements. To test the feasibility of this design, a 4 x 4 phoswich array was constructed, with each phoswich element consisting of two optically coupled, 3.17 x 1.58 x 10 mm(3) LSO crystals co-doped with cerium and calcium. The amount of calcium doping was varied to create a 'fast' LSO crystal with decay time of 32.9 ns and a 'slow' LSO crystal with decay time of 41.2 ns. Using a Hamamatsu R8900U-00-C12 position-sensitive photomultiplier tube (PS-PMT) and a CAEN V1720 250 MS/s waveform digitizer, we were able to show effective discrimination of the fast and slow LSO crystals in the phoswich array. Although a side-by-side phoswich array is feasible, reflections at the crystal boundary due to a mismatch between the refractive index of the optical adhesive (n = 1.5) and LSO ( n = 1.82) caused it to behave optically as an 8 x 4 array rather than a 4 x 4 array. Direct coupling of each phoswich element to individual photodetector elements may be necessary with the current phoswich array design. Alternatively, in order to implement this phoswich design with a conventional light sharing PET block detector, a high refractive index optical adhesive is necessary to closely match the refractive index of LSO. (C) 2017 Elsevier B.V. All rights reserved.
引用
收藏
页码:124 / 128
页数:5
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