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龟视网膜中视锥细胞之间的电耦合。

Electrical coupling between cones in turtle retina.

作者信息

Detwiler P B, Hodgkin A L

出版信息

J Physiol. 1979 Jun;291:75-100. doi: 10.1113/jphysiol.1979.sp012801.

Abstract
  1. The electrical coupling between cones of known spectral sensitivity in the peripheral part of the turtle's retina was studied by passing current through a micro-electrode inserted into one cone and recording with a second micro-electrode inserted into a neighbouring cone. 2. Spatial sensitivity profiles were determined by recording flash responses to a long narrow strip of light which was moved across the impaled cones in orthogonal directions. These measurements gave both the length constant lambda of electrical spread in the cone network and the separation of the two cones. 3. The cone separation determined from the spatial profiles agreed closely with that measured directly by injecting a fluorescent dye into two cones. 4. The length constant lambda varied from 18 to 39 micron with a mean of 25 micron for red-sensitive cones and 26 micron for green-sensitive cones. 5. The majority of cone pairs studied were electrically coupled provided they had the same spectral sensitivity and were separated by less than 60 micron: thirty-two out of thirty-six red-red pairs, two out of two green-green pairs, none out of eight red-green pairs: no blue cones were observed. 6. The strength of electrical coupling was expressed as a mutual resistance defined as the voltage in one cell divided by the current flowing into the other. Mutual resistances decreased from a maximum value of about 30 M omega at separations close to zero to 0.2 M omega, the lower limit of detectable coupling at separations of about 60 micron. Mutual resistances were always positive and were independent of which cell was directly polarized. The coupling seemed to be ohmic and any rectification or non-linearity probably arose in the cone membranes rather than in the coupling resistances. 7. The results were analysed in terms of the Lamb & Simon (1977) theories of square and hexagonal lattices, which approximate to the continuous sheet model except in the case of the cone to which current is applied. 8. The total membrane resistance of a single cone was estimated as 100--300 M omega and the connecting resistances as 100 M omega for a square array and 170 M omega for a hexagonal array. The input resistance of a cone in the network was 25--50 M omega. Lower values were often obtained but may be due to injury by the micro-electrodes. 9. The time constant of an isolated cone was estimated as about 20 msec and the capacity as about 100 pF. 10. Discrepancies between experimental findings and theoretical predictions of the hexagonal or square array models were tentatively attributed to an overestimate of lambda resulting from light scattering.
摘要
  1. 通过将电流通入插入一个视锥细胞的微电极,并使用插入相邻视锥细胞的另一个微电极进行记录,研究了海龟视网膜周边部分已知光谱敏感性视锥细胞之间的电耦合。2. 通过记录对视锥细胞垂直方向移动的狭长光带的闪光响应来确定空间敏感性分布。这些测量给出了视锥细胞网络中电传播的长度常数λ以及两个视锥细胞之间的间距。3. 从空间分布确定的视锥细胞间距与通过向两个视锥细胞中注入荧光染料直接测量的结果非常吻合。4. 长度常数λ在18至39微米之间变化,对红色敏感视锥细胞而言平均值为25微米,对绿色敏感视锥细胞而言为26微米。5. 所研究的大多数视锥细胞对在具有相同光谱敏感性且间距小于60微米时是电耦合的:36对红红视锥细胞对中有32对,2对绿绿视锥细胞对中有2对,8对红绿视锥细胞对中无一例;未观察到蓝色视锥细胞。6. 电耦合强度用互阻表示,互阻定义为一个细胞中的电压除以流入另一个细胞的电流。互阻从间距接近零时的最大值约30 MΩ降至0.2 MΩ,这是间距约60微米时可检测耦合的下限。互阻始终为正,且与哪个细胞直接极化无关。这种耦合似乎是欧姆性的,任何整流或非线性可能出现在视锥细胞膜而非耦合电阻中。7. 根据Lamb和Simon(1977年)的正方形和六边形晶格理论对结果进行了分析,除了施加电流的视锥细胞情况外,这些理论近似于连续片层模型。8. 单个视锥细胞的总膜电阻估计为100 - 300 MΩ,对于正方形阵列连接电阻为100 MΩ,对于六边形阵列连接电阻为170 MΩ。网络中视锥细胞的输入电阻为25 - 50 MΩ。经常获得较低的值,但这可能是由于微电极造成的损伤。9. 分离的视锥细胞的时间常数估计约为20毫秒,电容约为100 pF。10. 六边形或正方形阵列模型的实验结果与理论预测之间的差异暂时归因于光散射导致的λ估计过高。
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6080/1280889/d1c76a682f64/jphysiol00871-0106-a.jpg

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