Liu Zhongming, Kecman Fedja, He Bin
Department of Biomedical Engineering, University of Minnesota, 7-105 BSBE, 312 Church Street, Minneapolis, MN 55455, USA.
Clin Neurophysiol. 2006 Jul;117(7):1610-22. doi: 10.1016/j.clinph.2006.03.031. Epub 2006 Jun 9.
Multimodal functional neuroimaging by combining functional magnetic resonance imaging (fMRI) and electroencephalography (EEG) has been studied to achieve high-resolution reconstruction of the spatiotemporal cortical current density (CCD) distribution. However, mismatches between these two imaging modalities may occur due to their different underlying mechanisms. The aim of the present study is to investigate the effects of different types of fMRI-EEG mismatches, including fMRI invisible sources, fMRI extra regions and fMRI displacement, on the fMRI-constrained cortical imaging in a computer simulation based on realistic-geometry boundary-element-method (BEM) model.
Two methods have been adopted to integrate the synthetic fMRI and EEG data for CCD imaging. In addition to the well-known 90% fMRI-constrained Wiener filter approach (Liu AK, Belliveau JW, Dale AM. PNAS 1998;95:8945-8950.), we propose a novel two-step algorithm (referred to as 'Twomey algorithm') for fMRI-EEG integration. In the first step, a 'hard' spatial prior derived from fMRI is imposed to solve the EEG inverse problem with a reduced source space; in the second step, the fMRI constraint is removed and the source estimate from the first step is re-entered as the initial guess of the desired solution into an EEG least squares fitting procedure with Twomey regularization. Twomey regularization is a modified Tikhonov technique that attempts to simultaneously minimize the distance between the desired solution and the initial estimate, and the residual errors of fitness to EEG data. The performance of the proposed Twomey algorithm has been evaluated both qualitatively and quantitatively along with the lead-field normalized minimum norm (WMN) and the 90% fMRI-weighted Wiener filter approach, under repeated and randomized source configurations. Point spread function (PSF) and localization error (LE) are used to measure the performance of different imaging approaches with or without a variety of fMRI-EEG mismatches.
The results of the simulation show that the Twomey algorithm can successfully reduce the PSF of fMRI invisible sources compared to the Wiener estimation, without losing the merit of having much lower PSF of fMRI visible sources relative to the WMN solution. In addition, the existence of fMRI extra sources does not significantly affect the accuracy of the fMRI-EEG integrated CCD estimation for both the Wiener filter method and the proposed Twomey algorithm, while the Twomey algorithm may further reduce the chance of occurring spurious sources in the extra fMRI regions. The fMRI displacement away from the electrical source causes enlarged localization error in the imaging results of both the Twomey and Wiener approaches, while Twomey gives smaller LE than Wiener with the fMRI displacement ranging from 1-2 cm. With less than 2 cm fMRI displacement, the LEs for the Twomey and Wiener approaches are still smaller than in the WMN solution.
The present study suggests that the presence of fMRI invisible sources is the most problematic factor responsible for the error of fMRI-EEG integrated imaging based on the Wiener filter approach, whereas this approach is relatively robust against the fMRI extra regions and small displacement between fMRI activation and electrical current sources. While maintaining the above advantages possessed by the Wiener filter approach, the Twomey algorithm can further effectively alleviate the underestimation of fMRI invisible sources, suppress fMRI spurious sources and improve the robustness against fMRI displacement. Therefore, the Twomey algorithm is expected to improve the reliability of multimodal cortical source imaging against fMRI-EEG mismatches.
The proposed method promises to provide a useful alternative for multimodal neuroimaging integrating fMRI and EEG.
通过结合功能磁共振成像(fMRI)和脑电图(EEG)进行多模态功能神经成像,已被用于实现时空皮质电流密度(CCD)分布的高分辨率重建。然而,由于这两种成像方式的潜在机制不同,可能会出现不匹配的情况。本研究的目的是在基于真实几何边界元法(BEM)模型的计算机模拟中,研究不同类型的fMRI-EEG不匹配,包括fMRI不可见源、fMRI额外区域和fMRI位移,对fMRI约束皮质成像的影响。
采用两种方法将合成的fMRI和EEG数据进行整合以进行CCD成像。除了众所周知的90% fMRI约束维纳滤波器方法(Liu AK,Belliveau JW,Dale AM. PNAS 1998;95:8945 - 8950.),我们还提出了一种用于fMRI-EEG整合的新颖两步算法(称为“Twomey算法”)。第一步,施加从fMRI导出的“硬”空间先验,以在缩小的源空间中解决EEG逆问题;第二步,去除fMRI约束,并将第一步的源估计作为期望解的初始猜测重新输入到具有Twomey正则化的EEG最小二乘拟合过程中。Twomey正则化是一种改进的蒂霍诺夫技术,试图同时最小化期望解与初始估计之间的距离以及与EEG数据拟合的残差误差。在重复和随机的源配置下,已通过定性和定量方式评估了所提出的Twomey算法与导联场归一化最小范数(WMN)和90% fMRI加权维纳滤波器方法的性能。点扩散函数(PSF)和定位误差(LE)用于测量有无各种fMRI-EEG不匹配情况下不同成像方法的性能。
模拟结果表明,与维纳估计相比,Twomey算法能够成功降低fMRI不可见源的PSF,同时相对于WMN解,不会失去fMRI可见源PSF低得多的优点。此外,fMRI额外源的存在对维纳滤波器方法和所提出的Twomey算法的fMRI-EEG整合CCD估计的准确性没有显著影响,而Twomey算法可能会进一步降低在fMRI额外区域出现伪源的可能性。fMRI远离电源的位移会导致Twomey和维纳方法成像结果中的定位误差增大,而当fMRI位移在1 - 2 cm范围内时,Twomey的LE比维纳的小。当fMRI位移小于2 cm时,Twomey和维纳方法的LE仍小于WMN解中的LE。
本研究表明,fMRI不可见源的存在是基于维纳滤波器方法的fMRI-EEG整合成像误差的最主要问题因素,而该方法对fMRI额外区域以及fMRI激活与电流源之间的小位移具有相对较强的鲁棒性。在保持维纳滤波器方法上述优点的同时,Twomey算法可以进一步有效减轻对fMRI不可见源的低估,抑制fMRI伪源,并提高对fMRI位移的鲁棒性。因此,Twomey算法有望提高多模态皮质源成像针对fMRI-EEG不匹配的可靠性。
所提出的方法有望为整合fMRI和EEG的多模态神经成像提供一种有用的替代方法。