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快速稳态进动序列中的扰相梯度引起的扩散加权可能导致磁共振指纹成像中 T 测量不准确。

Diffusion-weighting Caused by Spoiler Gradients in the Fast Imaging with Steady-state Precession Sequence May Lead to Inaccurate T Measurements in MR Fingerprinting.

机构信息

Institute of Applied Physics, University of Tsukuba.

出版信息

Magn Reson Med Sci. 2019 Jan 10;18(1):96-104. doi: 10.2463/mrms.tn.2018-0027. Epub 2018 May 24.

DOI:10.2463/mrms.tn.2018-0027
PMID:29794408
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6326765/
Abstract

Magnetic resonance fingerprinting (MRF) is a promising framework that allows the quantification of multiple magnetic resonance parameters with a single scan. MRF using fast imaging with steady-state precession (MRF-FISP) has robustness to off-resonance artifacts and has many applications in inhomogeneous fields. However, the spoiler gradient used in MRF-FISP is sensitive to diffusion motion, and may lead to quantification errors when the spoiler moment increases. In this study, we examined the effect of the diffusion weighting in MRF-FISP caused by spoiler gradients. The T relaxation times were greatly underestimated when large spoiler moments were used. The T underestimation was prominent for tissues with large values of T and diffusion coefficients. The T bias was almost independent of the apparent diffusion coefficient (ADC) and T values when the ADC map was measured and incorporated into the matching process. These results reveal that the T underestimation resulted from the diffusion weighting caused by the spoiler gradients.

摘要

磁共振指纹成像(MRF)是一种很有前途的框架,可以在单次扫描中定量多个磁共振参数。使用稳态进动快速成像的 MRF(MRF-FISP)对离频伪影具有稳健性,并且在不均匀场中有许多应用。然而,MRF-FISP 中使用的扰断梯度对扩散运动很敏感,当扰断力矩增加时,可能会导致定量误差。在这项研究中,我们检查了扰断梯度在 MRF-FISP 中引起的扩散加权的影响。当使用大的扰断力矩时,T 弛豫时间会被大大低估。对于 T 值和扩散系数较大的组织,T 低估现象更为明显。当 ADC 图被测量并纳入匹配过程时,T 偏差几乎与表观扩散系数(ADC)和 T 值无关。这些结果表明,T 低估是由扰断梯度引起的扩散加权造成的。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/10f4868a02db/mrms-18-96-g7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/2c747c992f92/mrms-18-96-g1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/83c7363bb712/mrms-18-96-g2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/796782bc3cad/mrms-18-96-g3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/7a3361273734/mrms-18-96-g4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/5921ff327f57/mrms-18-96-g5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/014a72e230a6/mrms-18-96-g6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/10f4868a02db/mrms-18-96-g7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/2c747c992f92/mrms-18-96-g1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/83c7363bb712/mrms-18-96-g2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/796782bc3cad/mrms-18-96-g3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/7a3361273734/mrms-18-96-g4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/5921ff327f57/mrms-18-96-g5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/014a72e230a6/mrms-18-96-g6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dcd5/6326765/10f4868a02db/mrms-18-96-g7.jpg

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