To examine the kinetics of phototransduction in the living person, the electroretinogram (ERG) is measured in response to a family of moderately bright light intensities.
24 The a-wave of the rod ERG originates from the activity of the rod photoreceptors,
25 26 27 28 representing the rising phase of the rod photocurrent.
24 29 30 The behavior of the leading edge of the rod a-wave is similar to that of isolated rod photoreceptors in response to changes in intensity, wavelength, and adaptational state.
30 31 32 33 Because of these similarities, computational models describing the activation steps of phototransduction in isolated rod photoreceptors
30 have been applied to the leading edge of the rod a-wave measured in the living person.
34 These models are useful because, when used with care, parameters of rod a-wave activation measured in living humans can be associated with the activation of rod phototransduction. Relevant parameters include the maximum amplitude of the rod response (
Rm P3), a sensitivity parameter that scales the response as a function of flash intensity (
S), and a small delay before response onset of the rod response (
t d). Clinically, these models are useful, because the sensitivity and the maximum response of photoreceptors can be dissociated, which can reveal selective deficits, not detectable with the standard ERG.
35 For example, central vein occlusion decreases
S, whereas R
m P3 remains relatively stable.
35