Liang Z, Ye J, Harrington D P
Department of Radiology, State University of New York, Stony Brook, NY 11794, USA.
Phys Med Biol. 1994 Nov;39(11):2023-41. doi: 10.1088/0031-9155/39/11/014.
An analytical approach to quantitative brain SPECT (single-photon-emission computed tomography) with non-uniform attenuation is developed. The approach formulates accurately the projection-transform equation as a summation of primary- and scatter-photon contributions. The scatter contribution can be estimated using the multiple-energy-window samples and removed from the primary-energy-window data by subtraction. The approach models the primary contribution as a convolution of the attenuated source and the detector-response kernel at a constant depth from the detector with the central-ray approximation. The attenuated Radon transform of the source can be efficiently deconvolved using the depth-frequency relation. The approach inverts exactly the attenuated Radon transform by Fourier transforms and series expansions. The performance of the analytical approach was studied for both uniform- and non-uniform-attenuation cases, and compared to the conventional FBP (filtered-backprojection) method by computer simulations. A patient brain X-ray image was acquired by a CT (computed-tomography) scanner and converted to the object-specific attenuation map for 140 keV energy. The mathematical Hoffman brain phantom was used to simulate the emission source and was resized such that it was completely surrounded by the skull of the CT attenuation map. The detector-response kernel was obtained from measurements of a point source at several depths in air from a parallel-hole collimator of a SPECT camera. The projection data were simulated from the object-specific attenuating source including the depth-dependent detector response. Quantitative improvement (>5%) in reconstructing the data was demonstrated with the nonuniform attenuation compensation, as compared to the uniform attenuation correction and the conventional FBP reconstruction. The commuting time was less than 5 min on an HP/730 desktop computer for an image array of 128232 from 128 projections of 12832 size.
本文开发了一种针对非均匀衰减的定量脑单光子发射计算机断层扫描(SPECT)的分析方法。该方法将投影变换方程精确地表述为一次光子贡献和散射光子贡献的总和。散射贡献可通过多能量窗样本进行估计,并通过减法从一次能量窗数据中去除。该方法将一次贡献建模为衰减源与探测器响应核在距探测器恒定深度处的卷积,并采用中心射线近似。利用深度 - 频率关系可以有效地对源的衰减拉东变换进行反卷积。该方法通过傅里叶变换和级数展开精确地对衰减拉东变换进行反演。通过计算机模拟研究了该分析方法在均匀衰减和非均匀衰减情况下的性能,并与传统的滤波反投影(FBP)方法进行了比较。通过计算机断层扫描(CT)扫描仪获取患者脑部X射线图像,并将其转换为针对140keV能量的特定对象衰减图。使用数学霍夫曼脑模型模拟发射源,并调整其大小使其完全被CT衰减图的颅骨包围。探测器响应核是通过在SPECT相机的平行孔准直器的空气中几个深度处测量点源获得的。投影数据是从包括深度相关探测器响应的特定对象衰减源模拟得到的。与均匀衰减校正和传统FBP重建相比,非均匀衰减补偿在数据重建方面显示出定量改善(>5%)。对于128×32大小的128个投影生成的1282×32图像阵列,在HP/730台式计算机上的计算时间不到5分钟。