Light Adaptation of Retinal Rods, Adaptation Memory, and Afterimages

2020 ◽  
Vol 51 (1) ◽  
pp. 116-122
Author(s):  
A. Yu. Rotov ◽  
L. A. Astakhova ◽  
M. L. Firsov ◽  
V. I. Govardovskii
1991 ◽  
Vol 97 (3) ◽  
pp. 413-435 ◽  
Author(s):  
K Nakatani ◽  
T Tamura ◽  
K W Yau

The responses of rabbit rods to light were studied by drawing a single rod outer segment projecting from a small piece of retina into a glass pipette to record membrane current. The bath solution around the cells was maintained at near 40 degrees C. Light flashes evoked transient outward currents that saturated at up to approximately 20 pA. One absorbed photon produced a response of approximately 0.8 pA at peak. At the rising phase of the flash response, the relation between response amplitude and flash intensity (IF) had the exponential form 1-e-kappa FIF (where kappa F is a constant denoting sensitivity) expected from the absence of light adaptation. At the response peak, however, the amplitude-intensity relation fell slightly below the exponential form. At times after the response peak, the deviation was progressively more substantial. Light steps evoked responses that rose to a transient peak and rapidly relaxed to a lower plateau level. The response-intensity relation again indicated that light adaptation was insignificant at the early rising phase of the response, but became progressively more prominent at the transient peak and the steady plateau of the response. Incremental flashes superposed on a steady light of increasing intensity evoked responses that had a progressively shorter time-to-peak and faster relaxation, another sign of light adaptation. The flash sensitivity changed according to the Weber-Fechner relation (i.e., inversely) with background light intensity. We conclude that rabbit rods adapt to light in a manner similar to rods in cold-blooded vertebrates. Similar observations were made on cattle and rat rods.


1992 ◽  
Vol 55 ◽  
pp. 71
Author(s):  
L. Cervetto ◽  
S. Bisti ◽  
A. Campagni ◽  
S. Del Bianco ◽  
G.C. Demontis ◽  
...  

Nature ◽  
1988 ◽  
Vol 334 (6177) ◽  
pp. 69-71 ◽  
Author(s):  
K. Nakatani ◽  
K.-W. Yau

1990 ◽  
pp. 205-226
Author(s):  
S. Forti ◽  
A. Menini ◽  
G. Rispoli ◽  
L. Spadavecchia ◽  
V. Torre

1995 ◽  
Vol 69 (2) ◽  
pp. 439-450 ◽  
Author(s):  
G.C. Demontis ◽  
G.M. Ratto ◽  
S. Bisti ◽  
L. Cervetto

2005 ◽  
Vol 567 (3) ◽  
pp. 923-938 ◽  
Author(s):  
S. Nymark ◽  
H. Heikkinen ◽  
C. Haldin ◽  
K. Donner ◽  
A. Koskelainen

Science ◽  
1989 ◽  
Vol 245 (4919) ◽  
pp. 755-758 ◽  
Author(s):  
T Tamura ◽  
K Nakatani ◽  
K. Yau

1990 ◽  
Vol 96 (6) ◽  
pp. 1199-1220 ◽  
Author(s):  
C L Makino ◽  
L N Howard ◽  
T P Williams

Exposure of an intact vertebrate eye to light bleaches the rhodopsin in the photoreceptor outer segments in spatially nonuniform patterns. Some axial bleaching patterns produced in toad rods were determined using microspectrophotometric techniques. More rhodopsin was bleached at the base of the outer segment than at the distal tip. The shape of the bleaching gradient varied with the extent of bleach and with the spectral content of the illuminant. Monochromatic light at the lambda max of the rhodopsin gave rise to the steepest bleaching gradients and induced the greatest changes in the form of the gradient with increasing extent of bleach. These results were consistent with a mathematical model for pigment bleaching in an unstirred sample. The model did not fit bleaching patterns resulting from special lighting conditions that promoted the photoregeneration of rhodopsin from the intermediates of bleaching. Prolonged light adaptation of toads could also produce axial rhodopsin gradients that were not fit by the bleaching model. Under certain conditions the axial gradient of rhodopsin in a rod outer segment reversed with time in the light: the rhodopsin content became highest at the base. This result could be explained by an interaction between the pattern of bleaching and the intracellular topography of regeneration.


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