中国物理B ›› 2015, Vol. 24 ›› Issue (1): 18702-018702.doi: 10.1088/1674-1056/24/1/018702
• INTERDISCIPLINARY PHYSICS AND RELATED AREAS OF SCIENCE AND TECHNOLOGY • 上一篇 下一篇
樊馨a b, 王海鹏a b, 贠明凯a c, 孙校丽a b, 曹学香a c, 刘双全a c, 柴培a c, 李道武a c, 刘宝东a c, 王璐a b, 魏龙a c
Fan Xin (樊馨)a b, Wang Hai-Peng (王海鹏)a b, Yun Ming-Kai (贠明凯)a c, Sun Xiao-Li (孙校丽)a b, Cao Xue-Xiang (曹学香)a c, Liu Shuang-Quan (刘双全)a c, Chai Pei (柴培)a c, Li Dao-Wu (李道武)a c, Liu Bao-Dong (刘宝东)a c, Wang Lu (王璐)a b, Wei Long (魏龙)a c
摘要:
A point spread function (PSF) for the blurring component in positron emission tomography (PET) is studied. The PSF matrix is derived from the single photon incidence response function. A statistical iterative reconstruction (IR) method based on the system matrix containing the PSF is developed. More specifically, the gamma photon incidence upon a crystal array is simulated by Monte Carlo (MC) simulation, and then the single photon incidence response functions are calculated. Subsequently, the single photon incidence response functions are used to compute the coincidence blurring factor according to the physical process of PET coincidence detection. Through weighting the ordinary system matrix response by the coincidence blurring factors, the IR system matrix containing the PSF is finally established. By using this system matrix, the image is reconstructed by an ordered subset expectation maximization (OSEM) algorithm. The experimental results show that the proposed system matrix can substantially improve the image radial resolution, contrast, and noise property. Furthermore, the simulated single gamma-ray incidence response function depends only on the crystal configuration, so the method could be extended to any PET scanners with the same detector crystal configuration.
中图分类号: (Reconstruction)