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Effects of biological tissue structural anisotropy and anisotropy of magnetic susceptibility on the gradient echo MRI signal phase: theoretical background

机译:生物组织结构各向异性和磁化率各向异性对梯度回波MRI信号相位的影响:理论背景

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摘要

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.
机译:定量磁化率测绘是从梯度召回回波(GRE)MRI信号相位测绘组织磁化率的潜在强大技术。在这篇综述中,我们在分析GRE信号相位与基础组织微观结构和细胞磁化率之间的关系方面,提出了最新的理论进展。引起GRE信号相位的两个重要现象是本文的重点-组织结构各向异性(例如白质中的圆柱形轴突束)和磁化率各向异性。该领域中最引人入胜和最具挑战性的问题之一是计算所谓的洛伦兹(Lorentzian)对局部环境引起的相移的贡献–尺寸小于成像体素的磁化组织结构(例如细胞,细胞成分,毛细血管) 。在这篇综述中,我们将基于虚构的洛伦兹腔的引入,以及基于统计方法的最新洛伦兹张量方法(GLTA),简要讨论解决该问题的“标准”方法。静磁麦克斯韦方程的直接解。后者充分说明了两种类型的各向异性:磁化率的各向异性和结构组织的各向异性。在GLTA中,本地环境导致的频移的特征是洛伦兹张量 L ^ ,其结构与磁化张量<数学xmlns:mml =“ http://www.w3.org/1998/Math/MathML” display =“ inline” id =“ M2” overflow =“ scroll”> <移动器重音=“ true”> χ ^ 。而 <移动器重音=“ true” > χ ^ 是根据其体积分数“ <移动器重音=” true“> L ^ 由特定的数字因子加权,具体取决于组织的几何微观对称性。在多隔室结构中,洛伦兹张量的成分还取决于隔室的弛豫特性,因此取决于MR脉冲序列的设置。

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