Witzel Thomas, Lin Fa-Hsuan, Rosen Bruce R, Wald Lawrence L
Speech and Hearing Bioscience and Technology Program, Harvard-MIT Division of Health Sciences and Technology, USA.
Neuroimage. 2008 Oct 1;42(4):1357-65. doi: 10.1016/j.neuroimage.2008.05.010. Epub 2008 May 20.
Neuronal currents produce local transient and oscillatory magnetic fields that can be readily detected by MEG. Previous work attempting to detect these magnetic fields with MR focused on detecting local phase shifts and dephasing in T(2) or T(2)-weighted images. For temporally biphasic and multi-phasic local currents the sensitivity of these methods can be reduced through the cancellation of the accrued phase induced by positive and negative episodes of the neuronal current. The magnitude of the phase shift is also dependent on the distribution of the current within the voxel. Since spins on one side of a current source develop an opposite phase shift relative to those on the other side, there is likely to be significant cancellation within the voxel. We introduce a potential method for detecting neuronal currents though their resonant T(1rho) saturation during a spin-lock preparation period. The method is insensitive to the temporal and spatial cancellation effects since it utilizes the multi-phasic nature of the neuronal currents and thus is not sensitive to the sign of the local field. To produce a T(1)(rho) reduction, the Larmor frequency in the rotating frame, which is set by gammaB(1lock) (typically 20 Hz-5 kHz), must match the major frequency components of the stimulus-induced neuronal currents. We validate the method in MRI phantom studies. The rotary saturation spectra showed a sharp resonance when a current dipole within the phantom was driven at the Larmor frequency in the rotating frame. A 7 min block-design experiment was found to be sensitive to a current dipole strength of 56 nAm, an approximate magnetic field of 1 nT at 1.5 mm from the dipole. This dipole moment is similar to that seen using the phase shift method in a similar experimental setup by Konn et al. [Konn, D., Gowland, P., Bowtell, R., 2003. MRI detection of weak magnetic fields due to an extended current dipole in a conducting sphere: a model for direct detection of neuronal currents in the brain. Magn. Reson. Med. 50, 40-49], but is potentially less encumbered by temporal and spatial cancellation effects.
神经元电流会产生局部瞬态磁场和振荡磁场,这些磁场能够被脑磁图(MEG)轻易检测到。先前尝试用磁共振成像(MR)检测这些磁场的工作主要集中在检测T(2)或T(2)加权图像中的局部相位偏移和去相位。对于时间上双相和多相的局部电流,这些方法的灵敏度可能会因神经元电流正负相位引起的累积相位抵消而降低。相位偏移的大小还取决于体素内电流的分布。由于电流源一侧的自旋相对于另一侧的自旋会产生相反的相位偏移,因此在体素内很可能存在显著的抵消。我们介绍一种潜在的方法,即通过在自旋锁定准备期利用神经元电流的共振T(1rho)饱和来检测神经元电流。该方法对时间和空间抵消效应不敏感,因为它利用了神经元电流的多相性质,因此对局部场的符号不敏感。为了产生T(1)(rho)降低,旋转坐标系中的拉莫尔频率由gammaB(1lock)(通常为20 Hz - 5 kHz)设定,必须与刺激诱导的神经元电流的主要频率成分相匹配。我们在MRI体模研究中验证了该方法。当体模内的电流偶极以旋转坐标系中的拉莫尔频率驱动时,旋转饱和谱显示出尖锐的共振。发现一个7分钟的组块设计实验对强度为56 nAm的电流偶极敏感,在距偶极1.5 mm处的近似磁场为1 nT。这个偶极矩与Konn等人在类似实验设置中使用相位偏移方法所观察到的相似[Konn, D., Gowland, P., Bowtell, R., 2003. MRI detection of weak magnetic fields due to an extended current dipole in a conducting sphere: a model for direct detection of neuronal currents in the brain. Magn. Reson. Med. 50, 40 - 49],但可能受时间和空间抵消效应的影响较小。