Development of a novel depth of interaction PET detector using highly multiplexed G-APD cross-strip encoding

被引:23
作者
Kolb, A. [1 ]
Parl, C. [1 ]
Mantlik, F. [1 ,2 ]
Liu, C. C. [1 ]
Lorenz, E. [3 ]
Renker, D. [4 ]
Pichler, B. J. [1 ]
机构
[1] Univ Tubingen, Werner Siemens Imaging Ctr, Dept Preclin Imaging & Radiopharm, D-72076 Tubingen, Germany
[2] Max Planck Inst Intelligent Syst, Dept Empir Inference, D-72076 Tubingen, Germany
[3] Max Planck Inst Phys & Astrophys, D-80805 Munich, Germany
[4] Tech Univ Munich, Dept Phys, D-85748 Garching, Germany
关键词
PET; SiPM; DoT; PET/MRI; G-APD; POSITRON-EMISSION-TOMOGRAPHY; ENDED-SCINTILLATOR READOUT; CALIBRATE DOI FUNCTION; SMALL ANIMAL PET; HIGH-RESOLUTION; PERFORMANCE EVALUATION; SILICON PHOTOMULTIPLIER; SIMULTANEOUS PET/MRI; ECAT HRRT; SCANNER;
D O I
10.1118/1.4890609
中图分类号
R8 [特种医学]; R445 [影像诊断学];
学科分类号
1002 ; 100207 ; 1009 ;
摘要
Purpose: The aim of this study was to develop a prototype PET detector module for a combined small animal positron emission tomography and magnetic resonance imaging (PET/MR') system. The most important factor for small animal imaging applications is the detection sensitivity of the PET camera, which can be optimized by utilizing longer scintillation crystals. At the same time, small animal PET systems must yield a high spatial resolution. The measured object is very close to the PET detector because the bore.diameter of a high field animal MR scanner is limited. When used in combination with long scintillation crystals, these small-bore PET systems generate parallax errors that ultimately lead to a decreased spatial resolution. Thus, we developed a depth of interaction (DoI) encoding PET detector module that has a uniform spatial resolution across the whole field of view (FOY), high detection sensitivity, compactness, and insensitivity to magnetic fields. Methods: The approach was based on Geiger mode avalanche photodiode (G-APD) detectors with cross-strip encoding. The number of readout channels was reduced by a factor of 36 for the chosen block elements. Two 12 x 2 G-APD strip arrays (25 gm cells) were placed perpendicular on each face of a 12 x 12 lutetium oxyorthosilicate crystal block with a crystal size of 1.55 x 1.55 x 20 mm. The strip arrays were multiplexed into two channels and used to calculate the x, y coordinates for each array and the deposited energy. The DoT was measured in step sizes of 1.8 mm by a collimated 18F source. The coincident resolved time (CRT) was analyzed at all DoT positions by acquiring the waveform for each event and applying a digital leading edge discriminator. Results: All 144 crystals were well resolved in the crystal flood map. The average full width half maximum (FWHM) energy resolution of the detector was 12.8%+/- 1.5% with a FWHM CRT of 1.14 +/- 0.02 ns. The average FWHM DoI resolution over 12 crystals was 2.90 +/- 0.15 mm. Conclusions: The novel DoT PET detector, which is based on strip G-APD arrays, yielded a DoT resolution of 2.9 mm and excellent timing and energy resolution. Its high multiplexing factor reduces the number of electronic channels. Thus, this cross-strip approach enables low-cost, high-performance PET detectors for dedicated small animal PET and PET/MR' and potentially clinical PET/MRI systems. (C) 2014 American Association of Physicists in Medicine.
引用
收藏
页码:430 / 438
页数:9
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