Chen Guang-Hong, Leng Shuai, Mistretta Charles A
Department of Medical Physics, University of Wisconsin in Madison, Madison, Wisconsin 53704, USA.
Med Phys. 2005 Mar;32(3):654-65. doi: 10.1118/1.1861792.
The general goal of this paper is to extend the parallel-beam projection-slice theorem to divergent fan-beam and cone-beam projections without rebinning the divergent fan-beam and cone-beam projections into parallel-beam projections directly. The basic idea is to establish a novel link between the local Fourier transform of the projection data and the Fourier transform of the image object. Analogous to the two- and three-dimensional parallel-beam cases, the measured projection data are backprojected along the projection direction and then a local Fourier transform is taken for the backprojected data array. However, due to the loss of the shift invariance of the image object in a single view of the divergent-beam projections, the measured projection data is weighted by a distance dependent weight w(r) before the local Fourier transform is performed. The variable r in the weighting function w(r) is the distance from the backprojected point to the x-ray source position. It is shown that a special choice of the weighting function, w(r)=1/r, will facilitate the calculations and a simple relation can be established between the Fourier transform of the image function and the local Fourier transform of the 1/r-weighted backprojection data array. Unlike the parallel-beam cases, a one-to-one correspondence does not exist for a local Fourier transform of the backprojected data array and a single line in the two-dimensional (2D) case or a single slice in the 3D case of the Fourier transform of the image function. However, the Fourier space of the image object can be built up after the local Fourier transforms of the 1/r-weighted backprojection data arrays are shifted and then summed in a laboratory frame. Thus the established relations Eq. (27) and Eq. (29) between the Fourier space of the image object and the Fourier transforms of the backprojected data arrays can be viewed as a generalized projection-slice theorem for divergent fan-beam and cone-beam projections. Once the Fourier space of the image function is built up, an inverse Fourier transform could be performed to reconstruct tomographic images from the divergent beam projections. Due to the linearity of the Fourier transform, an image reconstruction step can be performed either when the complete Fourier space is available or in parallel with the building of the Fourier space. Numerical simulations are performed to verify the generalized projection-slice theorem by using a disc phantom in the fan-beam case.
本文的总体目标是将平行束投影切片定理扩展到发散扇形束和锥形束投影,而无需将发散扇形束和锥形束投影直接重新组合为平行束投影。基本思想是在投影数据的局部傅里叶变换与图像对象的傅里叶变换之间建立一种新颖的联系。类似于二维和三维平行束情况,将测量的投影数据沿投影方向进行反投影,然后对反投影数据阵列进行局部傅里叶变换。然而,由于在发散束投影的单个视图中图像对象的平移不变性丧失,在进行局部傅里叶变换之前,测量的投影数据由距离相关权重w(r)加权。加权函数w(r)中的变量r是从反投影点到x射线源位置的距离。结果表明,加权函数w(r)=1/r的特殊选择将便于计算,并且可以在图像函数的傅里叶变换与1/r加权反投影数据阵列的局部傅里叶变换之间建立简单的关系。与平行束情况不同,在二维情况下反投影数据阵列的局部傅里叶变换与图像函数傅里叶变换的一条线之间不存在一一对应关系,在三维情况下与一个切片之间也不存在一一对应关系。然而,在1/r加权反投影数据阵列的局部傅里叶变换进行移位然后在实验室坐标系中求和之后,可以构建图像对象的傅里叶空间。因此,在图像对象的傅里叶空间与反投影数据阵列的傅里叶变换之间建立的式(27)和式(29)关系可以被视为发散扇形束和锥形束投影的广义投影切片定理。一旦构建了图像函数的傅里叶空间,就可以进行傅里叶逆变换以从发散束投影重建断层图像。由于傅里叶变换的线性,可以在完整的傅里叶空间可用时执行图像重建步骤,或者与傅里叶空间的构建并行执行。通过在扇形束情况下使用圆盘模型进行数值模拟,以验证广义投影切片定理。