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评估盖革模式 APD 用于 PET 模块探测器设计。

Evaluation of Geiger-mode APDs for PET block detector designs.

机构信息

Department of Radiology, Laboratory for Preclinical Imaging and Imaging Technology of the Werner Siemens-Foundation, University of Tübingen, Röntgenweg 13, 72076 Tübingen, Germany.

出版信息

Phys Med Biol. 2010 Apr 7;55(7):1815-32. doi: 10.1088/0031-9155/55/7/003. Epub 2010 Mar 5.

Abstract

This paper presents an evaluation of two types of Geiger-mode avalanche photodiodes (G-APDs) for their potential to be used in a positron emission tomography (PET) detector. While the MPPC G-APD had only 3600 cells, the solid state photomultiplier (SSPM)-type G-APD had 8100 cells. In a single-channel G-APD/LSO setup, the energy resolution (DeltaEpsilon/Epsilon) of the SSPM at 511 keV was 25%, while the (DeltaEpsilon/Epsilon) of the MPPC was 13.5% (FWHM). No influences were observed while the detectors were inside a 7 T magnetic resonance (MR) scanner. A time resolution of 2.7 ns (FWHM) was measured for the LSO/SSPM and 0.9 ns for the LSO/MPPC detector setup. Although the linearity was superior for the SSPM in the single detector readout, the inferior energy and time resolution excluded them to be used for the block detector readout. All 12 x 12 LSO crystals of the block could be resolved in a crystal map using a 3 x 3 MPPC G-APD array. The time resolution of the block detector was 950 ps. While the energy spectra for the MPPC-based single-channel setup were nonlinear, they reached linearity better than 5% in the block detector. A high number of G-APD cells provide a linear signal in a single-channel detector setup, but not necessarily a good timing or (DeltaEpsilon/Epsilon) due to a larger inactive surface resulting in lower photon detection efficiency. G-APDs with a low number of cells provide a good timing and (DeltaEpsilon/Epsilon) and linear signals in block detector designs, where the scintillation light is shared over many G-APDs.

摘要

本文评估了两种类型的盖革模式雪崩光电二极管(G-APD),以评估它们在正电子发射断层扫描(PET)探测器中的应用潜力。虽然 MPPC G-APD 仅有 3600 个单元,但固态光电倍增管(SSPM)型 G-APD 则有 8100 个单元。在单通道 G-APD/LSO 设置中,SSPM 在 511keV 下的能量分辨率(ΔEpsilon/Epsilon)为 25%,而 MPPC 的(ΔEpsilon/Epsilon)为 13.5%(半高全宽)。当探测器在 7T 磁共振(MR)扫描仪内部时,没有观察到任何影响。LSO/SSPM 的时间分辨率为 2.7ns(半高全宽),LSO/MPPC 探测器设置的时间分辨率为 0.9ns。虽然在单探测器读取中 SSPM 的线性度更好,但较差的能量和时间分辨率排除了它们用于块状探测器读取。使用 3x3MPPCG-APD 阵列可以在晶体图中分辨出块状的所有 12x12LSO 晶体。块状探测器的时间分辨率为 950ps。虽然基于 MPPC 的单通道设置的能谱是非线性的,但在块状探测器中它们达到了优于 5%的线性度。在单通道探测器设置中,大量的 G-APD 单元提供线性信号,但由于较大的非活性表面导致光子探测效率降低,不一定能提供良好的定时或(ΔEpsilon/Epsilon)。在块状探测器设计中,具有少量单元的 G-APD 提供了良好的定时和(ΔEpsilon/Epsilon)以及线性信号,其中闪烁光在许多 G-APD 中共享。

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