The distribution of bumps in the tail of the locust photoreceptor afterpotential.

An extended tail or prolonged depolarizing afterpotential (PDA) follows the receptor potential of a locust retinula cell when the stimulating light is in the intensity range that saturates the receptor potential. The amplitude and duration of this afterpotential depend on the intensity and duration of the stimulus. As the afterpotential decays, apparently exponentially, it becomes resolved into bumps, which we call light-induced dark bumps (LID bumps). The intervals between light-induced dark bumps are distributed in a way that is indistinguishable from a random (Poisson) distribution. As previously demonstrated, LID bumps are indistinguishable from bumps directly induced by low intensity light in light-adapted cells, which in turn grade into the slightly larger bumps produced, each by a single photon, in dark-adapted cells. The light-induced dark bumps continue for up to an hour in darkness, slowly becoming like dark-adapted bumps in amplitude and shape. To account for the random occurrence and discrete features of bumps after so long a latency, we propose that intense light generates a significant amount of an intermediate molecule or packet which decays slowly to start the same process that normally generates bumps with a short delay.

[1]  S. Yeandle,et al.  Distribution of response times in visual sense cells after weak stimuli. , 1975, Journal of theoretical biology.

[2]  W. Pak,et al.  Induction of photoreceptor voltage noise in the dark in Drosophila mutant , 1975, Nature.

[3]  M. Cornwall,et al.  Ionic mechanism of a quasi‐stable depolarization in barnacle photoreceptor following red light. , 1975, The Journal of physiology.

[4]  K. Brown,et al.  Instrumentation and technique for beveling fine micropipette electrodes , 1975, Brain Research.

[5]  D. Stavenga,et al.  Photopigment conversions expressed in pupil mechanism of blowfly visual sense cells , 1975, Nature.

[6]  R. Srebro,et al.  A Stochastic Model for Discrete Waves in the Limulus Photoreceptor , 1971, The Journal of general physiology.

[7]  D. Baylor,et al.  Electrical responses of single cones in the retina of the turtle , 1970, The Journal of physiology.

[8]  M. Fuortes,et al.  Responses to single photons in visual cells of Limulus , 1968, The Journal of physiology.

[9]  J. Scholes,et al.  Discrete Subthreshold Potentials from the Dimly Lit Insect Eye , 1964, Nature.

[10]  M. Fuortes,et al.  Probability of Occurrence of Discrete Potential Waves in the Eye of Limulus , 1964, The Journal of general physiology.

[11]  B. Ninham,et al.  Theory of self-assembly of hydrocarbon amphiphiles into micelles and bilayers , 1976 .

[12]  F. Baumann,et al.  A depolarizing aftereffect of intense light in the drone visual receptor. , 1972, Vision research.

[13]  J. Scholes,et al.  Discontinuity of the excitation process in locust visual cells. , 1965, Cold Spring Harbor symposia on quantitative biology.