H. Tashima, E. Yoshida, Tetsuya Shinaji, T. Yamaya
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The head part has the shape of a cube. We set the center position of the asymmetric 2D Gaussian function at the center of the head part. The parameters of the asymmetric 2D Gaussian functions were calculated according to the size of the head part and tail part components perpendicular to the LOR. The proposed model was implemented on GPUs using the CUDA framework. We compared the proposed model with a simple Gaussian model and a crystal subsampling model which is an analytical model. We found DRFs in the proposed method provided a similar shape to that in the analytical model. In addition, the proposed model could include the blurring effect. The analytical model could represent only the effect of crystal shape, while the simple Gaussian model could represent only the blurring effect. Finally, the proposed method was applied for a prototype whole-body dual-ring OpenPET. As a result, the proposed method could improve the spatial resolution especially in the gap region of the OpenPET.","PeriodicalId":144711,"journal":{"name":"2014 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC)","volume":"22 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2014-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Detector response modeling with asymmetric 2D Gaussian functions for GPU-based image reconstruction of the whole-body dual-ring OpenPET\",\"authors\":\"H. Tashima, E. Yoshida, Tetsuya Shinaji, T. Yamaya\",\"doi\":\"10.1109/NSSMIC.2014.7430806\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We are developing the OpenPET which can provide an open space to make the patient observable and accessible during PET measurements. 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The proposed model was implemented on GPUs using the CUDA framework. We compared the proposed model with a simple Gaussian model and a crystal subsampling model which is an analytical model. We found DRFs in the proposed method provided a similar shape to that in the analytical model. In addition, the proposed model could include the blurring effect. The analytical model could represent only the effect of crystal shape, while the simple Gaussian model could represent only the blurring effect. Finally, the proposed method was applied for a prototype whole-body dual-ring OpenPET. 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引用次数: 0
摘要
我们正在开发OpenPET,它可以提供一个开放的空间,使患者在PET测量期间可以观察和接近。由于OpenPET几何结构具有许多斜响应线(LORs),因此实现OpenPET几何结构的关键技术之一是DOI (depth of interaction)探测器。即使DOI探测器降低了厚晶的模糊效应,但为了获得高空间分辨率图像,重建算法中对探测器响应函数(DRF)进行建模也是很重要的。因此,在本研究中,我们开发了一种新的基于垂直于LOR的非对称二维高斯函数的DRF模型,用于图形处理器在图像重建过程中的实时DRF计算。在提出的模型中,我们实际上将探测器晶体分为头和尾两部分。头部有一个立方体的形状。我们将非对称二维高斯函数的中心位置设置在头部的中心位置。根据垂直于LOR的头部和尾部分量的大小计算非对称二维高斯函数的参数。采用CUDA框架在gpu上实现了该模型。我们将该模型与简单高斯模型和晶体子采样模型进行了比较。我们发现该方法中的drf与解析模型中的drf具有相似的形状。此外,所提出的模型可以包括模糊效应。解析模型只能反映晶体形状的影响,而简单高斯模型只能反映模糊效应。最后,将该方法应用于一个全身双环OpenPET原型。结果表明,该方法可以提高OpenPET的空间分辨率,特别是在间隙区域。
Detector response modeling with asymmetric 2D Gaussian functions for GPU-based image reconstruction of the whole-body dual-ring OpenPET
We are developing the OpenPET which can provide an open space to make the patient observable and accessible during PET measurements. One of the key technologies for realizing the OpenPET geometry is the depth of interaction (DOI) detectors because the geometry has many oblique lines of response (LORs). Even if the DOI detectors reduce the blurring effect of the thick crystals, it is important to model the detector response function (DRF) in the reconstruction algorithm to achieve high spatial resolution images. In this study, therefore, we developed a new DRF model based on asymmetric 2D Gaussian functions perpendicular to the LOR for on-the-fly DRF calculation by GPUs during image reconstruction. In the proposed model, we virtually separated the detector crystal into two parts: head and tail. The head part has the shape of a cube. We set the center position of the asymmetric 2D Gaussian function at the center of the head part. The parameters of the asymmetric 2D Gaussian functions were calculated according to the size of the head part and tail part components perpendicular to the LOR. The proposed model was implemented on GPUs using the CUDA framework. We compared the proposed model with a simple Gaussian model and a crystal subsampling model which is an analytical model. We found DRFs in the proposed method provided a similar shape to that in the analytical model. In addition, the proposed model could include the blurring effect. The analytical model could represent only the effect of crystal shape, while the simple Gaussian model could represent only the blurring effect. Finally, the proposed method was applied for a prototype whole-body dual-ring OpenPET. As a result, the proposed method could improve the spatial resolution especially in the gap region of the OpenPET.