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本文引用的文献

1
Photometer for measuring intensity and rhodopsin distributions in intact eyes.用于测量完整眼睛中光强度和视紫红质分布的光度计。
Appl Opt. 1995 Sep 1;34(25):5720-4. doi: 10.1364/AO.34.005720.
2
QUANTUM RELATIONS OF THE RAT ELECTRORETINOGRAM.大鼠视网膜电图的量子关系
J Gen Physiol. 1963 Jul;46(6):1267-86. doi: 10.1085/jgp.46.6.1267.
3
The interpretation of spectral sensitivity curves.光谱灵敏度曲线的解读。
Br Med Bull. 1953;9(1):24-30. doi: 10.1093/oxfordjournals.bmb.a074302.
4
Visual transduction in human rod photoreceptors.人类视杆光感受器中的视觉转导。
J Physiol. 1993 May;464:747-65. doi: 10.1113/jphysiol.1993.sp019661.
5
Rod outer segment (ROS) renewal as a mechanism for adaptation to a new intensity environment. II. Rhodopsin synthesis and packing density.视杆外段(ROS)更新作为适应新强度环境的一种机制。二、视紫红质的合成与堆积密度。
Exp Eye Res. 1995 Jul;61(1):25-32. doi: 10.1016/s0014-4835(95)80055-7.
6
Rod outer segment (ROS) renewal as a mechanism for adaptation to a new intensity environment. I. Rhodopsin levels and ROS length.视杆细胞外段(ROS)更新作为一种适应新强度环境的机制。I. 视紫红质水平和ROS长度。
Exp Eye Res. 1995 Jul;61(1):17-23. doi: 10.1016/s0014-4835(95)80054-9.
7
Light distribution on the retina of a wide-angle theoretical eye.广角理论眼视网膜上的光分布。
J Opt Soc Am. 1983 Nov;73(11):1544-50. doi: 10.1364/josa.73.001544.
8
The photocurrent, noise and spectral sensitivity of rods of the monkey Macaca fascicularis.猕猴(食蟹猴)视杆细胞的光电流、噪声和光谱敏感性。
J Physiol. 1984 Dec;357:575-607. doi: 10.1113/jphysiol.1984.sp015518.
9
Encoding of nerve signals from retinal rods.来自视网膜视杆细胞的神经信号编码。
Nature. 1969 Sep 13;223(5211):1171-2. doi: 10.1038/2231171a0.
10
Photostasis: regulation of daily photon-catch by rat retinas in response to various cyclic illuminances.光稳态:大鼠视网膜对各种周期性光照强度的响应中对每日光子捕获的调节。
Exp Eye Res. 1986 Dec;43(6):915-28. doi: 10.1016/0014-4835(86)90070-9.

大鼠视网膜上光子吸收率的分布。

Distribution of photon absorption rates across the rat retina.

作者信息

Williams T P, Webbers J P, Giordano L, Henderson R P

机构信息

Department of Biological Science and Neuroscience Program, Florida State University, Tallahassee, FL 32306, USA.

出版信息

J Physiol. 1998 Apr 15;508 ( Pt 2)(Pt 2):515-22. doi: 10.1111/j.1469-7793.1998.515bq.x.

DOI:10.1111/j.1469-7793.1998.515bq.x
PMID:9508814
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC2230876/
Abstract
  1. An investigation into the distribution of light intensity across the rat retina was carried out on excised, intact rat eyes exposed to Ganzfeld illumination from a helium-neon laser (543 nm). 2. Some of the light entering the eyes exits through the sclera where its intensity can be monitored with an optical 'pick-up' that samples the intensity coming from a small region of external sclera and underlying retina. The spatial resolution of the pick-up is such that it samples light that has passed through ca 2 % of the rods in the rat eye. 3. Some of the laser light is absorbed by the rod pigment, rhodopsin, which gradually bleaches. Bleaching in the retina, in turn, causes an exponential increase in intensity emanating from the sclera. By monitoring this intensity increase, we are able to measure two important parameters in a single bleaching run: the local rhodopsin concentration and the local intensity falling on the rods. 4. With an ocular transmission photometer, we have measured both the local intensity and the local rhodopsin concentration across wide regions of rat retina. Both pigmented and albino rats were studied. 5. The distributions of rhodopsin and intensity were both nearly uniform; consequently, the product, (rhodopsin concentration) x (intensity), was similarly nearly equal across the retina. This means that the initial rate of photon absorption is about the same at all retinal locations. 6. Interpreted in terms of photostasis (the regulation of daily photon catch), this means that the rate of photon absorption is about the same in each rod, viz. 14 400 photons absorbed per rod per second. Since this rate of absorption is sufficient to saturate the rod, one possible purpose of photostasis is to maintain the rod system in a saturated state during daylight hours.
摘要
  1. 对暴露于氦氖激光(543纳米)全视野照明下的离体完整大鼠眼睛进行了一项关于大鼠视网膜光强度分布的研究。2. 进入眼睛的部分光线通过巩膜射出,其强度可通过一个光学“传感器”进行监测,该传感器对来自巩膜外部小区域及下方视网膜的强度进行采样。该传感器的空间分辨率使得它能对穿过大鼠眼中约2%视杆细胞的光线进行采样。3. 部分激光被视杆色素视紫红质吸收,视紫红质会逐渐漂白。视网膜中的漂白反过来会导致从巩膜发出的光强度呈指数增加。通过监测这种强度增加,我们能够在一次漂白过程中测量两个重要参数:局部视紫红质浓度和落在视杆细胞上的局部光强度。4. 使用眼透射光度计,我们测量了大鼠视网膜广泛区域的局部光强度和局部视紫红质浓度。研究了有色大鼠和白化大鼠。5. 视紫红质和光强度的分布几乎都是均匀的;因此,乘积(视紫红质浓度)×(光强度)在整个视网膜上同样几乎相等。这意味着在所有视网膜位置光子吸收的初始速率大致相同。6. 根据光稳态(每日光子捕获量的调节)来解释,这意味着每个视杆细胞中光子吸收的速率大致相同,即每秒每个视杆细胞吸收14400个光子。由于这种吸收速率足以使视杆细胞饱和,光稳态的一个可能目的是在白天使视杆系统保持在饱和状态。