Yablonskiy Dmitriy A, Sukstanskii Alexander L
Department of Radiology, Washington University, St Louis, MO, USA.
NMR Biomed. 2017 Apr;30(4). doi: 10.1002/nbm.3655. Epub 2016 Nov 11.
Quantitative susceptibility mapping is a potentially powerful technique for mapping tissue magnetic susceptibility from gradient recalled echo (GRE) MRI signal phase. In this review, we present up-to-date theoretical developments in analyzing the relationships between GRE signal phase and the underlying tissue microstructure and magnetic susceptibility at the cellular level. Two important phenomena contributing to the GRE signal phase are at the focus of this review - tissue structural anisotropy (e.g. cylindrical axonal bundles in white matter) and magnetic susceptibility anisotropy. One of the most intriguing and challenging problems in this field is calculating the so-called Lorentzian contribution to the phase shift induced by the local environment - magnetized tissue structures that have dimensions smaller than the imaging voxel (e.g. cells, cellular components, blood capillaries). In this review, we briefly discuss a "standard" approach to this problem, based on introduction of an imaginary Lorentzian cavity, as well as a more recent method - the generalized Lorentzian tensor approach (GLTA) - that is based on a statistical approach and a direct solution of the magnetostatic Maxwell equations. The latter adequately accounts for both types of anisotropy: the anisotropy of magnetic susceptibility and the structural tissue anisotropy. In the GLTA the frequency shift due to the local environment is characterized by the Lorentzian tensor L^, which has a substantially different structure than the susceptibility tensor χ^. While the components of χ^ are compartmental susceptibilities "weighted" by their volume fractions, the components of L^ are weighted by specific numerical factors depending on tissue geometrical microsymmetry. In multi-compartment structures, the components of the Lorentzian tensor also depend on the compartmental relaxation properties, hence the MR pulse sequence settings. Copyright © 2016 John Wiley & Sons, Ltd.
定量磁化率成像(QSM)是一种通过梯度回波(GRE)MRI信号相位来绘制组织磁化率的潜在强大技术。在本综述中,我们介绍了在细胞水平分析GRE信号相位与潜在组织微观结构及磁化率之间关系的最新理论进展。本综述重点关注导致GRE信号相位的两个重要现象——组织结构各向异性(如白质中的圆柱形轴突束)和磁化率各向异性。该领域最引人入胜且最具挑战性的问题之一是计算由局部环境(尺寸小于成像体素的磁化组织结构,如细胞、细胞成分、毛细血管)引起的相移的所谓洛伦兹贡献。在本综述中,我们简要讨论了基于引入虚洛伦兹腔的该问题的“标准”方法,以及一种更新的方法——广义洛伦兹张量方法(GLTA),它基于统计方法和静磁麦克斯韦方程的直接求解。后者充分考虑了两种各向异性:磁化率各向异性和组织结构各向异性。在GLTA中,由局部环境引起的频移由洛伦兹张量L^表征,其结构与磁化率张量χ^有很大不同。虽然χ^的分量是由其体积分数“加权”的隔室磁化率,但L^的分量由取决于组织几何微观对称性的特定数值因子加权。在多隔室结构中,洛伦兹张量的分量还取决于隔室弛豫特性,因此也取决于MR脉冲序列设置。版权所有© 2016 John Wiley & Sons, Ltd.