de Rochefort Ludovic, Nguyen Thanh, Brown Ryan, Spincemaille Pascal, Choi Grace, Weinsaft Jonathan, Prince Martin R, Wang Yi
Radiology Department, Weill Medical College of Cornell University, New York, New York 10022, USA.
Med Phys. 2008 Dec;35(12):5328-39. doi: 10.1118/1.3002309.
For pharmacokinetic modeling of tissue physiology, there is great interest in measuring the arterial input function (AIF) from dynamic contrast-enhanced (DCE) magnetic resonance imaging (MRI) using paramagnetic contrast agents. Due to relaxation effects, the measured signal is a nonlinear function of the injected contrast agent concentration and depends on sequence parameters, system calibration, and time-of-flight effects, making it difficult to accurately measure the AIF during the first pass. Paramagnetic contrast agents also affect susceptibility and modify the magnetic field in proportion to their concentration. This information is contained in the MR signal phase which is discarded in a typical image reconstruction. However, quantifying AIF through contrast agent susceptibility induced phase changes is made difficult by the fact that the induced magnetic field is nonlocal and depends upon the contrast agent spatial distribution and thus on organ and vessel shapes. In this article, the contrast agent susceptibility was quantified through inversion of magnetic field shifts using a piece-wise constant model. Its feasibility is demonstrated by a determination of the AIF from the susceptibility-induced field changes of an intravenous bolus. After in vitro validation, a time-resolved two-dimensional (2D) gradient echo scan, triggered to diastole, was performed in vivo on the aortic arch during a bolus injection of 0.1 mmol/kg Gd-DTPA. An approximate geometrical model of the aortic arch constructed from the magnitude images was used to calculate the spatial variation of the field associated with the bolus. In 14 subjects, Gd concentration curves were measured dynamically (one measurement per heart beat) and indirectly validated by independent 2D cine phase contrast flow rate measurements. Flow rate measurements using indicator conservation with this novel quantitative susceptibility imaging technique were found to be in good agreement with those obtained from the cine phase contrast measurements in all subjects. Contrary to techniques that rely on intensity, the accuracy of this signal phase based method is insensitive to factors influencing signal intensity such as flip angle, coil sensitivity, relaxation changes, and time-of-flight effects extending the range of pulse sequences and contrast doses for which quantitative DCE-MRI can be applied.
对于组织生理学的药代动力学建模,人们对使用顺磁性造影剂通过动态对比增强(DCE)磁共振成像(MRI)测量动脉输入函数(AIF)有着浓厚的兴趣。由于弛豫效应,所测量的信号是注入造影剂浓度的非线性函数,并且取决于序列参数、系统校准和飞行时间效应,这使得在首次通过期间准确测量AIF变得困难。顺磁性造影剂还会影响磁化率,并与其浓度成比例地改变磁场。该信息包含在MR信号相位中,而在典型的图像重建中该相位会被舍弃。然而,由于感应磁场是非局部的,并且取决于造影剂的空间分布,进而取决于器官和血管的形状,通过造影剂磁化率诱导的相位变化来量化AIF变得困难。在本文中,使用分段常数模型通过磁场偏移反演来量化造影剂磁化率。通过从静脉推注的磁化率诱导场变化确定AIF证明了其可行性。经过体外验证后,在静脉注射0.1 mmol/kg Gd-DTPA期间,在体内对主动脉弓进行了触发至舒张期的时间分辨二维(2D)梯度回波扫描。由幅度图像构建的主动脉弓近似几何模型用于计算与推注相关的场的空间变化。在14名受试者中,动态测量了Gd浓度曲线(每心跳一次测量一次),并通过独立的2D电影相位对比流速测量进行了间接验证。发现使用这种新型定量磁化率成像技术通过指示剂守恒进行的流速测量与所有受试者通过电影相位对比测量获得的结果高度一致。与依赖强度的技术相反,这种基于信号相位的方法的准确性对影响信号强度的因素(如翻转角、线圈灵敏度、弛豫变化和飞行时间效应)不敏感,从而扩展了可应用定量DCE-MRI的脉冲序列和造影剂剂量范围。