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猫视网膜Y细胞的感受野空间结构。

The receptive-field spatial structure of cat retinal Y cells.

作者信息

Enroth-Cugell C, Freeman A W

机构信息

Biomedical Engineering Division, Northwestern University, Evanston, IL 60201.

出版信息

J Physiol. 1987 Mar;384:49-79. doi: 10.1113/jphysiol.1987.sp016443.

DOI:10.1113/jphysiol.1987.sp016443
PMID:3656154
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC1192251/
Abstract
  1. Y-type ganglion cells in the cat's retina were stimulated with bars of light and grating patterns at photopic luminances. Stimuli were stationary, and luminance at each point was varied sinusoidally in time at 2 Hz. Impulse rates were recorded from single cells. 2. When the stimulus was a narrow bar of light, the impulse rate approached a sinusoidal function of time as contrast was reduced. The linear behaviour of each cell was therefore characterized by taking the limit of response parameters as contrast approached zero. 3. The ratio of surround strength to centre strength varied widely between cells but the two strengths were approximately equal on average. The difference between surround phase and centre phase averaged 168 deg. 4. As contrast increased, responses became rectified. Rectifier output was well described by a power law of stimulus amplitude, where the power was usually 1.4 or 1.5. 5. Response phase advanced with increasing contrast, and at high response amplitudes grew less than proportionally with contrast. These effects were assumed due to the contrast gain control described by Shapley & Victor (1978). 6. Gratings in which luminance varied sinusoidally with distance were used to determine Y cell spatial resolution. The second-harmonic amplitude of the response diminished rapidly with increasing spatial frequency: the radius of the best-fitting Gaussian mechanism was about 0.25 deg for a cell at 10 deg eccentricity. 7. This spatial resolution is close to the linear resolution of X cells as determined by Linsenmeier, Frishman, Jakiela & Enroth-Cugell (1982). 8. A receptive field model incorporating both linear and non-linear elements is described. The model consists of an array of subunit pathways, each of which has a centre-surround organization followed by a rectifier; a pool weights and sums subunit outputs, and signals are then passed through a contrast gain control. 9. The model accounts qualitatively for the over-all centre-surround organization of Y cell linear responses, the dependence of frequency-doubled responses on spatial frequency, and impulse rate as a function of time for a variety of bar and grating stimuli.
摘要
  1. 在明视觉亮度下,用条形光和光栅图案刺激猫视网膜中的Y型神经节细胞。刺激物是静止的,每个点的亮度随时间以2赫兹的频率呈正弦变化。记录单个细胞的冲动发放率。2. 当刺激物是一条窄的条形光时,随着对比度降低,冲动发放率接近时间的正弦函数。因此,每个细胞的线性行为通过将对比度接近零时响应参数的极限来表征。3. 细胞之间,周边强度与中心强度的比值差异很大,但平均而言,这两种强度大致相等。周边相位与中心相位的差异平均为168度。4. 随着对比度增加,响应变为整流。整流器输出可以通过刺激幅度的幂律很好地描述,其中幂通常为1.4或1.5。5. 响应相位随着对比度增加而提前,并且在高响应幅度下,其增长与对比度不成正比。这些效应被认为是由于Shapley和Victor(1978年)描述的对比度增益控制所致。6. 使用亮度随距离呈正弦变化的光栅来确定Y细胞的空间分辨率。响应的二次谐波幅度随着空间频率的增加而迅速减小:对于偏心度为10度的细胞,最佳拟合高斯机制的半径约为0.25度。7. 这种空间分辨率接近Linsenmeier、Frishman、Jakiela和Enroth-Cugell(1982年)确定的X细胞的线性分辨率。8. 描述了一个包含线性和非线性元件的感受野模型。该模型由一系列亚单位通路组成,每个通路都有一个中心-周边组织,随后是一个整流器;一个池对亚单位输出进行加权和求和,然后信号通过对比度增益控制。9. 该模型定性地解释了Y细胞线性响应的整体中心-周边组织、倍频响应对空间频率的依赖性以及各种条形和光栅刺激下冲动发放率随时间的变化。
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2f2d/1192251/5400ff5a6bd0/jphysiol00536-0082-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2f2d/1192251/9e1ea83e8386/jphysiol00536-0071-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2f2d/1192251/5400ff5a6bd0/jphysiol00536-0082-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2f2d/1192251/9e1ea83e8386/jphysiol00536-0071-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2f2d/1192251/5400ff5a6bd0/jphysiol00536-0082-a.jpg

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2
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J Physiol. 1960 Oct;153(3):583-94. doi: 10.1113/jphysiol.1960.sp006557.
3
How the contrast gain control modifies the frequency responses of cat retinal ganglion cells.对比度增益控制如何改变猫视网膜神经节细胞的频率响应。
光感受器丧失对视网膜环路的影响。
Annu Rev Vis Sci. 2021 Sep 15;7:105-128. doi: 10.1146/annurev-vision-100119-124713.
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