Pierpaoli C, Basser P J
Neuroimaging Branch, National Institute of Neurological Diseases and Stroke (NINDS), Bethesda, Maryland 20892, USA.
Magn Reson Med. 1996 Dec;36(6):893-906. doi: 10.1002/mrm.1910360612.
Indices of diffusion anisotropy calculated from diffusion coefficients acquired in two or three perpendicular directions are rotationally variant. In living monkey brain, these indices severely underestimate the degree of diffusion anisotropy. New indices calculated from the entire diffusion tensor are rotationally invariant (RI). They show that anisotropy is highly variable in different white matter regions depending on the degree of coherence of fiber tract directions. In structures with a regular, parallel fiber arrangement, water diffusivity in the direction parallel to the fibers (Dparallel approximately 1400-1800 x 10(-6) mm2/s) is almost 10 times higher than the average diffusivity in directions perpendicular to them (D + D)/2 [corrected] approximately 150-300 x 10(-6) mm2/s), and is almost three times higher than previously reported. In structures where the fiber pattern is less coherent (e.g., where fiber bundles merge), diffusion anisotropy is significantly reduced. However, RI anisotropy indices are still susceptible to noise contamination. Monte Carlo simulations show that these indices are statistically biased, particularly those requiring sorting of the eigenvalues of the diffusion tensor based on their magnitude. A new intervoxel anisotropy index is proposed that locally averages inner products between diffusion tensors in neighboring voxels. This "lattice" RI index has an acceptably low error variance and is less susceptible to bias than any other RI anisotropy index proposed to date.
根据在两个或三个垂直方向获取的扩散系数计算得到的扩散各向异性指数是旋转可变的。在活体猴脑中,这些指数严重低估了扩散各向异性的程度。从整个扩散张量计算得到的新指数是旋转不变的(RI)。它们表明,根据纤维束方向的相干程度,不同白质区域的各向异性变化很大。在具有规则平行纤维排列的结构中,平行于纤维方向的水扩散率(D平行约为1400 - 1800×10⁻⁶mm²/s)几乎比垂直于纤维方向的平均扩散率((D + D)/2[校正后]约为150 - 300×10⁻⁶mm²/s)高10倍,并且几乎比之前报道的高3倍。在纤维模式相干性较低的结构中(例如纤维束合并的地方),扩散各向异性显著降低。然而,RI各向异性指数仍然容易受到噪声污染。蒙特卡罗模拟表明,这些指数存在统计偏差,特别是那些需要根据扩散张量特征值大小进行排序的指数。提出了一种新的体素间各向异性指数,该指数对相邻体素中的扩散张量内积进行局部平均。这种“晶格”RI指数具有可接受的低误差方差,并且比迄今为止提出的任何其他RI各向异性指数更不易受到偏差的影响。