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本文引用的文献

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Whole brain susceptibility mapping using compressed sensing.全脑磁化率成像的压缩感知技术。
Magn Reson Med. 2012 Jan;67(1):137-47. doi: 10.1002/mrm.23000. Epub 2011 Jun 10.
2
A computational multiresolution BOLD fMRI model.计算多分辨率 BOLD fMRI 模型。
IEEE Trans Biomed Eng. 2011 Oct;58(10):2995-9. doi: 10.1109/TBME.2011.2158823. Epub 2011 Jun 7.
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Two pitfalls of BOLD fMRI magnitude-based neuroimage analysis: non-negativity and edge effect.基于 BOLD fMRI 幅度的神经影像分析的两个陷阱:非负性和边缘效应。
J Neurosci Methods. 2011 Aug 15;199(2):363-9. doi: 10.1016/j.jneumeth.2011.05.018. Epub 2011 May 26.
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Quantitative susceptibility mapping of human brain reflects spatial variation in tissue composition.人脑的定量磁化率映射反映了组织成分的空间变化。
Neuroimage. 2011 Apr 15;55(4):1645-56. doi: 10.1016/j.neuroimage.2010.11.088. Epub 2011 Jan 9.
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Quantitative imaging of intrinsic magnetic tissue properties using MRI signal phase: an approach to in vivo brain iron metabolism?利用 MRI 信号相位对固有磁组织特性进行定量成像:一种用于活体脑铁代谢的方法?
Neuroimage. 2011 Feb 14;54(4):2789-807. doi: 10.1016/j.neuroimage.2010.10.070. Epub 2010 Oct 30.
6
Susceptibility mapping as a means to visualize veins and quantify oxygen saturation.作为可视化静脉和量化氧饱和度的手段的敏感图。
J Magn Reson Imaging. 2010 Sep;32(3):663-76. doi: 10.1002/jmri.22276.
7
Susceptibility mapping in the human brain using threshold-based k-space division.基于阈值的 K 空间分区的人脑易感性图绘制。
Magn Reson Med. 2010 May;63(5):1292-304. doi: 10.1002/mrm.22334.
8
Quantitative susceptibility map reconstruction from MR phase data using bayesian regularization: validation and application to brain imaging.基于贝叶斯正则化从磁共振相位数据重建定量磁化率图:验证及在脑成像中的应用
Magn Reson Med. 2010 Jan;63(1):194-206. doi: 10.1002/mrm.22187.
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Magnetic susceptibility mapping of brain tissue in vivo using MRI phase data.利用 MRI 相位数据对活体脑组织进行磁化率映射。
Magn Reson Med. 2009 Dec;62(6):1510-22. doi: 10.1002/mrm.22135.
10
Nonlinear regularization for per voxel estimation of magnetic susceptibility distributions from MRI field maps.基于 MRI 场图对每体素磁化率分布进行非线性正则化估计。
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用于磁共振成像图重建的计算机逆共振成像

Computed inverse resonance imaging for magnetic susceptibility map reconstruction.

作者信息

Chen Zikuan, Calhoun Vince

机构信息

The Mind Research Network, University of New Mexico, Albuquerque, NM 87106, USA.

出版信息

J Comput Assist Tomogr. 2012 Mar-Apr;36(2):265-74. doi: 10.1097/RCT.0b013e3182455cab.

DOI:10.1097/RCT.0b013e3182455cab
PMID:22446372
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4347950/
Abstract

OBJECTIVE

This article reports a computed inverse magnetic resonance imaging (CIMRI) model for reconstructing the magnetic susceptibility source from MRI data using a 2-step computational approach.

METHODS

The forward T2*-weighted MRI (T2MRI) process is broken down into 2 steps: (1) from magnetic susceptibility source to field map establishment via magnetization in the main field and (2) from field map to MR image formation by intravoxel dephasing average. The proposed CIMRI model includes 2 inverse steps to reverse the T2MRI procedure: field map calculation from MR-phase image and susceptibility source calculation from the field map. The inverse step from field map to susceptibility map is a 3-dimensional ill-posed deconvolution problem, which can be solved with 3 kinds of approaches: the Tikhonov-regularized matrix inverse, inverse filtering with a truncated filter, and total variation (TV) iteration. By numerical simulation, we validate the CIMRI model by comparing the reconstructed susceptibility maps for a predefined susceptibility source.

RESULTS

Numerical simulations of CIMRI show that the split Bregman TV iteration solver can reconstruct the susceptibility map from an MR-phase image with high fidelity (spatial correlation ≈ 0.99). The split Bregman TV iteration solver includes noise reduction, edge preservation, and image energy conservation. For applications to brain susceptibility reconstruction, it is important to calibrate the TV iteration program by selecting suitable values of the regularization parameter.

CONCLUSIONS

The proposed CIMRI model can reconstruct the magnetic susceptibility source of T2*MRI by 2 computational steps: calculating the field map from the phase image and reconstructing the susceptibility map from the field map. The crux of CIMRI lies in an ill-posed 3-dimensional deconvolution problem, which can be effectively solved by the split Bregman TV iteration algorithm.

摘要

目的

本文报道一种计算逆磁共振成像(CIMRI)模型,该模型使用两步计算方法从MRI数据重建磁化率源。

方法

正向T2加权MRI(T2MRI)过程分为两步:(1)通过主磁场中的磁化从磁化率源到场图建立;(2)通过体素内去相位平均从场图到MR图像形成。所提出的CIMRI模型包括两个逆步骤以反转T2*MRI过程:从MR相位图像计算场图以及从场图计算磁化率源。从场图到磁化率图的逆步骤是一个三维不适定反卷积问题,可通过三种方法解决:Tikhonov正则化矩阵求逆、带截断滤波器的逆滤波以及全变差(TV)迭代。通过数值模拟,我们通过比较预定义磁化率源的重建磁化率图来验证CIMRI模型。

结果

CIMRI的数值模拟表明,分裂Bregman TV迭代求解器能够以高保真度(空间相关性≈0.99)从MR相位图像重建磁化率图。分裂Bregman TV迭代求解器包括降噪、边缘保留和图像能量守恒。对于脑磁化率重建应用,通过选择合适的正则化参数值来校准TV迭代程序很重要。

结论

所提出的CIMRI模型可通过两个计算步骤重建T2*MRI的磁化率源:从相位图像计算场图以及从场图重建磁化率图。CIMRI的关键在于一个不适定的三维反卷积问题,该问题可通过分裂Bregman TV迭代算法有效解决。