多对比磁共振血管磁粒子成像弛豫谱分析。

Relaxation spectral analysis in multi-contrast vascular magnetic particle imaging.

机构信息

CAS Key Laboratory of Molecular Imaging, Beijing Key Laboratory of Molecular Imaging, The State Key Laboratory of Management and Control for Complex Systems, Institute of Automation, Chinese Academy of Sciences, Beijing, China.

School of Computer Science and Technology, Xidian University, Xi'an, Shaanxi, China.

出版信息

Med Phys. 2023 Jul;50(7):4651-4663. doi: 10.1002/mp.16551. Epub 2023 Jun 9.

Abstract

BACKGROUND

Magnetic nanoparticles (MNPs) are used as tracers without ionizing radiation in vascular imaging, molecular imaging, and neuroimaging. The relaxation mechanisms of magnetization in response to excitation magnetic fields are important features of MNPs. The basic relaxation mechanisms include internal rotation (Néel relaxation) and external physical rotation (Brownian relaxation). Accurate measurement of these relaxation times may provide high sensitivity for predicting MNP types and viscosity-based hydrodynamic states. It is challenging to separately measure the Néel and Brownian relaxation components using sinusoidal excitation in conventional MPI.

PURPOSE

We developed a multi-exponential relaxation spectral analysis method to separately measure the Néel and Brownian relaxation times in the magnetization recovery process in pulsed vascular MPI.

METHODS

Synomag-D samples with different viscosities were excited using pulsed excitation in a trapezoidal-waveform relaxometer. The samples were excited at different field amplitudes ranging from 0.5 to 10 mT at intervals of 0.5 mT. The inverse Laplace transform-based spectral analysis of the relaxation-induced decay signal in the field-flat phase was performed by using PDCO, a primal-dual interior method for convex objectives. Néel and Brownian relaxation peaks were elucidated and measured on samples with various glycerol and gelatin concentrations. The sensitivity of viscosity prediction of the decoupled relaxation times was evaluated. A digital vascular phantom was designed to mimic a plaque with viscous MNPs and a catheter with immobilized MNPs. Spectral imaging of the digital vascular phantom was simulated by combining a field-free point with homogeneous pulsed excitation. The relationship between the Brownian relaxation time from different tissues and the number of periods for signal averages was evaluated for a scan time estimation in the simulation.

RESULTS

The relaxation spectra of synomag-D samples with different viscosity levels exhibited two relaxation time peaks. The Brownian relaxation time had a positive linear relationship with the viscosity in the range 0.9 to 3.2 mPa · s. When the viscosity was >3.2 mPa · s, the Brownian relaxation time saturated and did not change with increasing viscosity. The Néel relaxation time decreased slightly with an increase in the viscosity. The Néel relaxation time exhibited a similar saturation effect when the viscosity level was >3.2 mPa · s for all field amplitudes. The sensitivity of the Brownian relaxation time increased with the field amplitude and was maximized at approximately 4.5 mT. The plaque and catheter regions were differentiated from the vessel region in the simulated Brownian relaxation time map. The simulation results show that the Néel relaxation time was 8.33±0.09 μs in the plaque region, 8.30±0.08 μs in the catheter region, and 8.46±0.11 μs in the vessel region. The Brownian relaxation time was 36.60±2.31 μs in the plaque region, 30.17±1.24 μs in the catheter region, and 31.21±1.53 μs in the vessel region. If we used 20 excitation periods for image acquisition in the simulation, the total scan time of the digital phantom was approximately 100 s.

CONCLUSION

Quantitative assessment of the Néel and Brownian relaxation times through inverse Laplace transform-based spectral analysis in pulsed excitation, highlighting their potential for use in multi-contrast vascular MPI.

摘要

背景

磁性纳米粒子(MNPs)在血管成像、分子成像和神经成像中用作无电离辐射示踪剂。磁化对激励磁场的弛豫机制是 MNPs 的重要特征。基本弛豫机制包括内部旋转(奈尔弛豫)和外部物理旋转(布朗弛豫)。准确测量这些弛豫时间可以为预测 MNP 类型和基于粘度的流体动力学状态提供高灵敏度。在传统的 MPI 中,使用正弦激励分别测量奈尔和布朗弛豫分量具有挑战性。

目的

我们开发了一种多指数弛豫谱分析方法,用于在脉冲血管 MPI 中的磁化恢复过程中分别测量奈尔和布朗弛豫时间。

方法

使用梯形波弛豫仪对具有不同粘度的 Synomag-D 样品进行脉冲激励。样品在 0.5 至 10 mT 的场振幅范围内以 0.5 mT 的间隔进行激励。通过使用 PDCO(用于凸目标的原始对偶内部方法)对场平坦相中的弛豫诱导衰减信号进行基于逆拉普拉斯变换的谱分析。在具有不同甘油和明胶浓度的样品上阐明和测量了奈尔和布朗弛豫峰。评估了分离弛豫时间的粘度预测的灵敏度。设计了一个数字血管仿体,以模拟具有粘性 MNPs 的斑块和具有固定 MNPs 的导管。通过结合自由点和均匀脉冲激励来模拟数字血管仿体的光谱成像。评估了不同组织的布朗弛豫时间与信号平均周期数之间的关系,以便在模拟中估计扫描时间。

结果

具有不同粘度水平的 Synomag-D 样品的弛豫谱显示出两个弛豫时间峰。布朗弛豫时间与 0.9 至 3.2 mPa·s 范围内的粘度呈正线性关系。当粘度>3.2 mPa·s 时,布朗弛豫时间饱和且不随粘度增加而变化。随着粘度的增加,奈尔弛豫时间略有下降。当所有场振幅的粘度水平>3.2 mPa·s 时,奈尔弛豫时间表现出类似的饱和效应。布朗弛豫时间的灵敏度随场振幅增加,并在约 4.5 mT 时达到最大值。在模拟的布朗弛豫时间图中,斑块和导管区域与血管区域区分开来。模拟结果表明,斑块区域的奈尔弛豫时间为 8.33±0.09 μs,导管区域为 8.30±0.08 μs,血管区域为 8.46±0.11 μs。斑块区域的布朗弛豫时间为 36.60±2.31 μs,导管区域为 30.17±1.24 μs,血管区域为 31.21±1.53 μs。如果我们在模拟中使用 20 个激励周期进行图像采集,则数字仿体的总扫描时间约为 100 s。

结论

通过脉冲激励中的基于逆拉普拉斯变换的谱分析定量评估奈尔和布朗弛豫时间,突出了它们在多对比度血管 MPI 中的应用潜力。

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