Robert S Miyaoka, Xiaoli Li, Cate Lockhart, Tom K Lewellen
{"title":"Design of a High Resolution, Monolithic Crystal, PET/MRI Detector with DOI Positioning Capability.","authors":"Robert S Miyaoka, Xiaoli Li, Cate Lockhart, Tom K Lewellen","doi":"10.1109/NSSMIC.2008.4774469","DOIUrl":null,"url":null,"abstract":"<p><p>We report on a high resolution, monolithic crystal PET detector design concept that provides depth of interaction (DOI) positioning within the crystal and is compatible for operation in a MRI scanner to support multimodal anatomic and functional imaging. Our design utilizes a novel sensor on the entrance surface (SES) approach combined with a maximum likelihood positioning algorithm. The sensor will be a two-dimensional array of micro-pixel avalanche photodiodes (MAPD). MAPDs are a new type of solid-state photodetector with Geiger mode operation that can provide signal gain similar to a photomltipiler tube (PMT). In addition, they can be operated in high magnetic fields to support PET/MR imaging. Utilizing a multi-step simulation process, we determined the intrinsic spatial resolution characteristics for a variety of detector configurations. The crystal was always modeled as a 48.8 mm by 48.8 mm by 15 mm monolithic slab of a lutetium-based scintillator. The SES design was evaluated via simulation for three different two-dimensional MAPD array sizes: 8×8 with 5.8×5.8 mm(2) pads; 12×12 with 3.8×3.8 mm(2) pads; and 16×16 with 2.8×2.8 mm(2) pads. To reduce the number of signal channels row-column summing readout was explored for the 12×12 and 16×16 channel array devices. The intrinsic spatial resolution for the 8×8 MAPD array is 0.88 mm FWHM in X and Y, and 1.83 mm FWHM in Z (i.e., DOI). Comparing the results versus using a conventional design with the photosensors on the backside of the crystal, an average improvement of ~24% in X and Y and 20% in Z is achieved. The X, Y intrinsic spatial resolution improved to 0.66 mm and 0.65 mm FWHM for the 12×12 and 16×16 MAPDs using row-column readout. Using the 12×12 and 16×16 arrays also led to a slight improvement in the DOI positioning accuracy.</p>","PeriodicalId":73298,"journal":{"name":"IEEE Nuclear Science Symposium conference record. Nuclear Science Symposium","volume":" ","pages":"4688-4692"},"PeriodicalIF":0.0000,"publicationDate":"2008-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1109/NSSMIC.2008.4774469","citationCount":"10","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Nuclear Science Symposium conference record. Nuclear Science Symposium","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/NSSMIC.2008.4774469","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 10
Abstract
We report on a high resolution, monolithic crystal PET detector design concept that provides depth of interaction (DOI) positioning within the crystal and is compatible for operation in a MRI scanner to support multimodal anatomic and functional imaging. Our design utilizes a novel sensor on the entrance surface (SES) approach combined with a maximum likelihood positioning algorithm. The sensor will be a two-dimensional array of micro-pixel avalanche photodiodes (MAPD). MAPDs are a new type of solid-state photodetector with Geiger mode operation that can provide signal gain similar to a photomltipiler tube (PMT). In addition, they can be operated in high magnetic fields to support PET/MR imaging. Utilizing a multi-step simulation process, we determined the intrinsic spatial resolution characteristics for a variety of detector configurations. The crystal was always modeled as a 48.8 mm by 48.8 mm by 15 mm monolithic slab of a lutetium-based scintillator. The SES design was evaluated via simulation for three different two-dimensional MAPD array sizes: 8×8 with 5.8×5.8 mm(2) pads; 12×12 with 3.8×3.8 mm(2) pads; and 16×16 with 2.8×2.8 mm(2) pads. To reduce the number of signal channels row-column summing readout was explored for the 12×12 and 16×16 channel array devices. The intrinsic spatial resolution for the 8×8 MAPD array is 0.88 mm FWHM in X and Y, and 1.83 mm FWHM in Z (i.e., DOI). Comparing the results versus using a conventional design with the photosensors on the backside of the crystal, an average improvement of ~24% in X and Y and 20% in Z is achieved. The X, Y intrinsic spatial resolution improved to 0.66 mm and 0.65 mm FWHM for the 12×12 and 16×16 MAPDs using row-column readout. Using the 12×12 and 16×16 arrays also led to a slight improvement in the DOI positioning accuracy.
我们报告了一种高分辨率的单片晶体PET检测器设计概念,该设计概念在晶体内提供相互作用深度(DOI)定位,并与MRI扫描仪中的操作兼容,以支持多模态解剖和功能成像。我们的设计采用了一种新型的入口表面传感器(SES)方法,结合了最大似然定位算法。传感器将是一个微像素雪崩光电二极管(MAPD)的二维阵列。mapd是一种具有盖革模式操作的新型固态光电探测器,可以提供类似于光电倍增管(PMT)的信号增益。此外,它们可以在高磁场下操作,以支持PET/MR成像。利用多步模拟过程,我们确定了各种探测器配置的固有空间分辨率特征。该晶体一直被建模为一个基于镥的闪烁体的48.8 mm × 48.8 mm × 15 mm的单片板。SES设计通过模拟评估了三种不同的二维MAPD阵列尺寸:8×8与5.8×5.8 mm(2)的衬垫;12×12带3.8×3.8 mm(2)垫片;和16×16与2.8×2.8毫米(2)垫片。为了减少信号通道的数量,探索了12×12和16×16通道阵列器件的行列求和读出。8×8 MAPD阵列在X和Y方向的固有空间分辨率为0.88 mm FWHM,在Z方向(即DOI)的固有空间分辨率为1.83 mm FWHM。与在晶体背面安装光传感器的传统设计相比,在X和Y上平均提高了24%,在Z上平均提高了20%。使用行-列读出方式,12×12和16×16 mapd的X, Y固有空间分辨率分别提高到0.66 mm和0.65 mm FWHM。使用12×12和16×16阵列也导致DOI定位精度略有提高。