Kaufman L, Okada Y, Brenner D, Williamson S J
Int J Neurosci. 1981;15(4):223-39. doi: 10.3109/00207458108985860.
Recently Okada et al. (1981) reported that stimulation of the median nerve with a brief electrical impulse at the wrist evoked a transient change in the brain's magnetic field. This somatic evoked field (SEF) is similar in its temporal waveform to the response to the same stimulus reported for the electrical potential recorded on the pial surface of the exposed brain. Moreover, both measures differ substantially from the somatic evoked potential (SEP) recorded at the scalp. The present paper describes a more detailed account of the SEF as well as an analysis of its relation to the SEP and to the somatic pial response (SPR). Its purpose of the use the three measures in clarifying our understanding of the nature and locations of sources of the SEF. This paper is divided into three sections. The first is a background section which reviews basic principles and models that are widely used in deducing the locations of sources of evoked potentials and fields. It indicates the types of currents which may give rise to the SEF, and distinguishes between them and the current which is associated with the SEP. It concludes with a rationale for the experiments described in the next section. The experiments described in the second section determined how the SEF varies with the position from which it is recorded at the scalp. These variations turn out to be essential to our understanding of the nature and location of the sources of the SEF. The third section summarizes the results of the experiments and makes clear how they affect theories of the origin of the SEF. The findings also have implications for our understanding of the SEP and SPR. The most salient findings are: (1) The SEF recorded normal to the head provides essentially the same information as that provided by reported potential recordings from the exposed surface of the brain (the SPR). (2) The SEF originates in the cortex of the cerebrum in the vicinity of the central sulcus. (3) The currents that account for identifiable components of the SEF are opposite in direction to those that account for corresponding components of the SPR. This result is consistent with models that ascribe the detected field normal to the scalp to intracellular currents, whereas the VEP is associated with extracellular currents flowing in the opposite direction.
最近,冈田等人(1981年)报告称,在手腕处用短暂电脉冲刺激正中神经会引起大脑磁场的短暂变化。这种躯体诱发电场(SEF)的时间波形与在暴露大脑的软脑膜表面记录的相同刺激的电位反应相似。此外,这两种测量方法与在头皮处记录的躯体诱发电位(SEP)有很大不同。本文详细描述了SEF,并分析了它与SEP以及躯体软脑膜反应(SPR)的关系。使用这三种测量方法的目的是为了更清楚地理解SEF的性质和来源位置。本文分为三个部分。第一部分是背景部分,回顾了在推导诱发电位和电场来源位置时广泛使用的基本原理和模型。它指出了可能产生SEF的电流类型,并将它们与与SEP相关的电流区分开来。最后给出了下一部分所述实验的理论依据。第二部分描述的实验确定了SEF如何随在头皮上记录它的位置而变化。这些变化对于我们理解SEF的性质和来源位置至关重要。第三部分总结了实验结果,并阐明了它们如何影响SEF起源的理论。这些发现对我们理解SEP和SPR也有启示。最显著的发现是:(1)垂直于头部记录的SEF提供的信息与从暴露的大脑表面记录的电位(SPR)提供的信息基本相同。(2)SEF起源于中央沟附近的大脑皮层。(3)构成SEF可识别成分的电流方向与构成SPR相应成分的电流方向相反。这一结果与将垂直于头皮检测到的场归因于细胞内电流的模型一致,而VEP与相反方向流动的细胞外电流相关。