Department of Biomedical Engineering, Wayne State University, United States of America.
Department of Radiology, Wayne State University, United States of America.
Magn Reson Imaging. 2019 Sep;61:196-206. doi: 10.1016/j.mri.2019.05.006. Epub 2019 May 10.
When an object contains a distribution of discrete magnetic inclusions with a constant susceptibility, the MRI signal inside the object may no longer be determined analytically by assuming that the object is uniform or magnetic inclusions are completely random. Through simulations and experiments with spherical particles inside cylinders, this work is to study the signal behavior in the static dephasing regime.
MRI complex images of long cylinders containing spherical particles with different arrangements were simulated and compared to similar experimental phantom data. All experiments were designed for the static dephasing regime so that diffusion was neglected.
Several factors can lead to different phase shifts over echo time. These include numbers of particles per image voxel, particle arrangements, and Gibbs ringing effects. Purely random arrangements of particles in simulations can agree with a revised theoretical formula at short echo times, but quasi-random arrangements of particles do not agree with the theory. In addition, close to half of experimental results show deviations from the theory and the quasi-random arrangements of particles can explain those experimental results. Simulated R values are about the same for different cylinder orientations but increase when random particle arrangement is restricted toward lattice. Nonetheless, as expected, phase distributions outside and far away from each cylinder are independent of any factor affecting phase inside and behave as if they are from a cylinder with a uniform bulk susceptibility.
Phase over echo time inside an object containing discrete spheres can be nonlinear and deviate from current theories in the static dephasing regime. Phase outside the object can be used to accurately determine its magnetic moment and bulk susceptibility without a priori knowledge of the spherical particle distribution inside the object. These results can be extended to the subcortical gray matter and suggest that in vivo susceptibility quantification will need to be re-thought.
当物体包含具有恒定磁化率的离散磁性夹杂物分布时,通过假设物体是均匀的或磁性夹杂物是完全随机的,物体内部的 MRI 信号可能不再可以通过分析确定。通过在圆柱体内进行球形粒子的模拟和实验,这项工作旨在研究静态去相位状态下的信号行为。
模拟了具有不同排列的长圆柱体内含有球形粒子的 MRI 复杂图像,并将其与类似的实验体模数据进行了比较。所有实验均设计为静态去相位状态,因此忽略了扩散。
几个因素可能导致不同的相位在回波时间上的变化。这些因素包括每个图像体素中的粒子数、粒子排列和吉布斯振铃效应。在模拟中,粒子的纯随机排列可以在短回波时间内与修正后的理论公式一致,但粒子的准随机排列则不符合理论。此外,接近一半的实验结果偏离了理论,而粒子的准随机排列可以解释这些实验结果。模拟的 R 值对于不同的圆柱取向大致相同,但当随机粒子排列受到限制时,它们会增加。不过,正如预期的那样,圆柱体外部和远处的相位分布与影响内部相位的任何因素无关,并且表现得好像它们来自具有均匀体磁化率的圆柱体。
在包含离散球体的物体内部,随着回波时间的变化,相位可能是非线性的,并且在静态去相位状态下可能偏离当前理论。物体外部的相位可用于在无需事先了解物体内部球形粒子分布的情况下准确确定其磁矩和体磁化率。这些结果可以扩展到皮质下灰质,并表明体内磁化率定量将需要重新考虑。