Molecular Imaging Center, National Institute of Radiological Sciences, 4-9-1 Anagawa, Inage-ku, Chiba 263-8555, Japan.
Phys Med Biol. 2011 Nov 7;56(21):6793-807. doi: 10.1088/0031-9155/56/21/003. Epub 2011 Oct 5.
We are developing a novel, general purpose isotropic-3D PET detector X'tal cube which has high spatial resolution in all three dimensions. The research challenge for this detector is implementing effective detection of scintillation photons by covering six faces of a segmented crystal block with silicon photomultipliers (SiPMs). In this paper, we developed the second prototype of the X'tal cube for a proof-of-concept. We aimed at realizing an ultimate detector with 1.0 mm(3) cubic crystals, in contrast to our previous development using 3.0 mm(3) cubic crystals. The crystal block was composed of a 16 × 16 × 16 array of lutetium gadolinium oxyorthosilicate (LGSO) crystals 0.993 × 0.993 × 0.993 mm(3) in size. The crystals were optically glued together without inserting any reflector inside and 96 multi-pixel photon counters (MPPCs, S10931-50P, i.e. six faces each with a 4 × 4 array of MPPCs), each having a sensitive area of 3.0 × 3.0 mm(2), were optically coupled to the surfaces of the crystal block. Almost all 4096 crystals were identified through Anger-type calculation due to the finely adjusted reflector sheets inserted between the crystal block and light guides. The reflector sheets, which formed a belt of 0.5 mm width, were placed to cover half of the crystals of the second rows from the edges in order to improve identification performance of the crystals near the edges. Energy resolution of 12.7% was obtained at 511 keV with almost uniform light output for all crystal segments thanks to the effective detection of the scintillation photons.
我们正在开发一种新型的、通用的各向同性 3D PET 探测器 X'tal cube,它在所有三个维度上都具有高空间分辨率。该探测器的研究挑战是通过用硅光电倍增管 (SiPM) 覆盖分段晶体块的六个面来有效检测闪烁光子。在本文中,我们开发了 X'tal cube 的第二个原型,用于概念验证。我们的目标是实现一个具有 1.0 mm(3)立方晶体的终极探测器,与我们之前使用 3.0 mm(3)立方晶体的开发相比。晶体块由一个 16 × 16 × 16 阵列的硅酸镥钆氧(LGSO)晶体组成,尺寸为 0.993 × 0.993 × 0.993 mm(3)。晶体之间没有插入任何反射器,而是通过光学胶合在一起,96 个多像素光子计数器(MPPC,S10931-50P,即每个面有一个 4 × 4 阵列的 MPPC),每个具有 3.0 × 3.0 mm(2)的敏感面积,与晶体块的表面光学耦合。由于在晶体块和光导之间插入了精细调整的反射片,几乎所有 4096 个晶体都可以通过 Anger 型计算来识别。反射片形成了一个 0.5 毫米宽的带,放置在边缘的第二行的一半晶体上,以提高边缘附近晶体的识别性能。由于闪烁光子的有效检测,在 511keV 处获得了 12.7%的能量分辨率,所有晶体段的光输出几乎均匀。