Nakagawa H, Miyazaki H, Matsumoto N
Department of Biochemical Engineering and Science, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Fukuoka, Japan.
Vis Neurosci. 1997 Mar-Apr;14(2):263-75. doi: 10.1017/s0952523800011408.
In the frog optic tectum, the spatiotemporal pattern of neuronal activity evoked by electrical stimulation of the optic tract was examined by means of a current source density (CSD) analysis. The CSD depth profile was highly reproducible in different experiments. In all seven CSD profiles, three current sinks A, B, and D were observed in the retinorecipient layers. Four out of the seven profiles show additional two sinks C and E below the retinorecipient layers. Very small and short lasting sinks related to afferent fiber activities precede sinks A and B by about 1 ms, which could be accounted for by monosynaptic delay, in the corresponding depth region. The earliest prominent sink A at the bottom of the retinorecipient layers reflects only excitatory monosynaptic activities derived from R3 and/or R4 retinal ganglion cells. The second prominent sink B in the superficial retinorecipient layer is composed partly of excitatory monosynaptic activity from medium-sized myelinated optic fibers. It may involve excitatory monosynaptic activity from unmyelinated optic fibers and further polysynaptic activity. The fourth prominent sink D in the intermediate retinorecipient layer partially reflects excitatory monosynaptic activity derived from unmyelinated optic fibers. It may also involve further polysynaptic activity. In contrast with these three sinks, the third prominent sink C and fifth sink E exclusively reflect intratectal polysynaptic activity that has not been reported in any previous CSD studies in the frog optic tectum. These sinks almost overlap spatially in the tectal layer. We also measured the intratectal resistance changes and computed inhomogeneous CSD depth profiles to show that the results from homogeneous CSD computation assuming constant conductivity are valid for our present study. Finally, we compared the present results with previously reported CSD studies on the frog optic tectum and discuss consistencies and discrepancies among these experiments.
在青蛙视顶盖中,通过电流源密度(CSD)分析方法研究了对视神经束进行电刺激所诱发的神经元活动的时空模式。CSD深度分布在不同实验中具有高度可重复性。在所有七个CSD分布图中,在视网膜接受层观察到三个电流汇A、B和D。七个分布图中有四个在视网膜接受层下方还显示出另外两个电流汇C和E。与传入纤维活动相关的非常小且持续时间短的电流汇在相应深度区域比电流汇A和B提前约1毫秒出现,这可以用单突触延迟来解释。视网膜接受层底部最早出现的明显电流汇A仅反映来自R3和/或R4视网膜神经节细胞的兴奋性单突触活动。视网膜接受层浅层的第二个明显电流汇B部分由来自中等大小有髓鞘视神经纤维的兴奋性单突触活动组成。它可能涉及来自无髓鞘视神经纤维的兴奋性单突触活动以及进一步的多突触活动。视网膜接受层中间层的第四个明显电流汇D部分反映来自无髓鞘视神经纤维的兴奋性单突触活动。它也可能涉及进一步的多突触活动。与这三个电流汇不同,第三个明显电流汇C和第五个电流汇E仅反映视顶盖内多突触活动,这在之前青蛙视顶盖的任何CSD研究中均未报道。这些电流汇在顶盖层中几乎在空间上重叠。我们还测量了视顶盖内的电阻变化并计算了非均匀CSD深度分布,以表明假设电导率恒定的均匀CSD计算结果对我们目前的研究是有效的。最后,我们将目前的结果与之前报道的关于青蛙视顶盖的CSD研究进行了比较,并讨论了这些实验之间的一致性和差异。