磁化率源与t2*图像在形态上的不匹配。

Magnetic resonance insights Pub Date : 2013-08-01 eCollection Date: 2013-01-01 DOI:10.4137/MRI.S11920
Zikuan Chen, Vince Calhoun
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引用次数: 20

摘要

背景和目的:最近的研究表明,T2*图像(无论是幅度还是相位)与磁化率(χ)源的内部空间分布不相同。在本文中,我们通过研究T2*加权磁共振成像(T2*MRI)的见解来研究这些差异背后的原因,并通过数值模拟提供源/像不匹配的数值表征。方法:对于T2*MRI的数值模拟,我们预先定义了一个3D χ源,并通过在存在和不存在扩散的情况下进行体内消相来计算复值T2*图像。我们提出了一个经验α-功率模型来描述整个源/像转换。对于高斯形χ源,我们根据空间相关性和FWHM(最大一半时的全宽度)对源/图像形态不匹配进行了数值表征。结果:理论上,我们发现由于偶极子效应,χ-诱导的场图在形态上与χ源不同,T2*级图像在小相角区域通过二次变换与场图相关,这施加了额外的形态变化。高斯型χ源的数值模拟表明,T2*级图像可能会遭受20%至25%的整体源/图像形态收缩,并且T2*相位图像与田野图几乎相同,因此由于偶极子效应而与χ源保持形态不匹配。结论:块体χ源与T2*图像的形态不匹配是由组织磁化过程中的三维卷积(偶极子效应)、T2*大小和相位计算的非线性以及自旋扩散效应引起的。在小相角状态下,T2*星等整体形态收缩,T2*相图像受到偶极子效应的影响,但仍保持χ-诱导的场图形态。
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Understanding the morphological mismatch between magnetic susceptibility source and t2* image.

Background and purpose: Recent research has shown that a T2* image (either magnitude or phase) is not identical to the internal spatial distribution of a magnetic susceptibility (χ) source. In this paper, we examine the reasons behind these differences by looking into the insights of T2*-weighted magnetic resonance imaging (T2*MRI) and provide numerical characterizations of the source/image mismatches by numerical simulations.

Methods: For numerical simulations of T2*MRI, we predefine a 3D χ source and calculate the complex-valued T2* image by intravoxel dephasing in presence and absence of diffusion. We propose an empirical α-power model to describe the overall source/image transformation. For a Gaussian-shaped χ source, we numerically characterize the source/image morphological mismatch in terms of spatial correlation and FWHM (full width at half maximum).

Results: In theory, we show that the χ-induced fieldmap is morphologically different from the χ source due to dipole effect, and the T2* magnitude image is related to the fieldmap by a quadratic transformation in the small phase angle regime, which imposes an additional morphological change. The numerical simulations with a Gaussian-shaped χ source show that a T2* magnitude image may suffer an overall source/image morphological shrinkage of 20% to 25% and that the T2* phase image is almost identical to the fieldmap thus maintaining a morphological mismatch from the χ source due to dipole effect.

Conclusion: The morphological mismatch between a bulk χ source and its T2* image is caused by the 3D convolution during tissue magnetization (dipole effect), the nonlinearity of the T2* magnitude and phase calculation, and the spin diffusion effect. In the small phase angle regime, the T2* magnitude exhibits an overall morphological shrinkage, and the T2* phase image suffers a dipole effect but maintains the χ-induced fieldmap morphology.

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