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Light adaptation and dark adaptation of human rod photoreceptors measured from the a-wave of the electroretinogram

机译:从视网膜电图的a波测得的人体棒状光感受器的光适应和暗适应

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class="enumerated" style="list-style-type:decimal">We recorded the a-wave of the human electroretinogram from subjects with normal vision, using a corneal electrode and ganzfeld (full-field) light stimulation. From analysis of the rising phase of rod-isolated flash responses we determined the maximum size (amax) of the a-wave, a measure of the massed circulating current of the rods, and the amplification constant (A) of transduction within the rod photoreceptors.During light adaptation by steady backgrounds the maximal response was reduced, as reported previously. amax declined approximately as I0/(I0+IB), where IB is retinal illuminance and I0 is a constant. In different subjects I0 ranged from 40 to 100 trolands, with a mean of 70 trolands, corresponding to about 600 photoisomerizations s−1 per rod. (1 troland is the retinal illuminance that results when a surface luminance of 1 cd m−2 is viewed through a pupil area of 1 mm2.) The amplification constant A decreased only slightly in the presence of steady backgrounds.Following a full bleach amax recovered along an S-shaped curve over a period of 30 min. There was no detectable response for the first 5 min, and half-maximal recovery took 13-17 min.The apparent amplification constant decreased at early times after large bleaches. However, upon correction for reduced light absorption due to loss of pigment, with regeneration of rhodopsin occurring with a time constant of 9-15 min in different subjects, it appeared that the true value of A was probably unchanged by bleaching.The recovery of amax following a bleach could be converted into recovery of equivalent background intensity, using a ‘Crawford transformation’ derived from the light adaptation results. Following bleaches ranging from 10 to > 99 %, the equivalent background intensity decayed approximately exponentially, with a time constant of about 3 min.The time taken for amax to recover to a fixed proportion of its original level increased approximately linearly (rather than logarithmically) with fractional bleach, with a slope of about 12 min per 100 % bleach. Similar behaviour has previously been seen in psychophysical dark adaptation experiments, for the dependence of the ‘second component’ of recovery on the level of bleaching.
机译:class =“ enumerated” style =“ list-style-type:decimal”> <!-list-behavior =枚举前缀-word = mark-type = decimal max-label-size = 0-> 我们使用角膜电极和ganzfeld(全视野)光刺激记录了正常视力受试者的人体视网膜电图a波。通过对杆隔离闪光响应的上升阶段的分析,我们确定了a波的最大大小(amax),杆的质量循环电流的量度以及杆感光器内转导的放大常数(A)。 如前所述,在稳定背景下的光适应过程中,最大响应降低了。 amax大约下降为I0 /(I0 + IB),其中IB是视网膜照度,I0是常数。在不同的对象中,I0为40至100 troland,平均为70 troland,对应于每根棒约600次光异构化s -1 。 (1 troland是当通过1 mm 2 的瞳孔区域观察到1 cd m -2 的表面亮度时所产生的视网膜照度。)放大常数A减小 在充满漂白剂的情况下,在30分钟内沿着S形曲线恢复了最大漂白峰。在开始的5分钟内没有可检测到的响应,并且最大恢复时间为13-17分钟。 在大漂白后的早期,表观扩增常数下降。然而,经过校正以减少由于色素损失引起的光吸收,视紫红质的再生以不同的时间常数在9-15分钟之间发生,在不同的受试者中,看来A的真实值可能不会因漂白而改变。使用从光适应结果得出的“克劳福德变换”,可以将漂白后的amax的恢复转化为等效背景强度的恢复。从10%到> 99%的漂白,当量背景强度大约以指数衰减,时间常数约为3分钟。 使max恢复到其原始水平的固定比例所花费的时间增加了与部分漂白剂近似线性(而不是对数),每100%漂白剂的斜率约为12分钟。以前在心理生理暗适应实验中已经发现了类似的行为,这是恢复的“第二部分”对漂白水平的依赖性。

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