Purpose
To test the hypothesis that a simple model having properties consistent with activation and deactivation in the rod approximates the whole time course of the photoresponse.
Methods
Routinely, an exponential of the form
f
=
α
·(1 – exp(–(
τ
·(
t
–
t
eff
)
s
–1
))), with amplitude
α
, rate constant
τ
(often scaled by intensity), irreducible delay
t
eff
, and time exponent
s
–1, is fit to the early period of the flash electroretinogram. Notably,
s
(an integer) represents the three integrating stages in the rod amplification cascade (rhodopsin isomerization, transducin activation, and cGMP hydrolysis). The time course of the photoresponse to a 0.17 cd·s·m
−2
conditioning flash (CF) was determined in 21 healthy eyes by presenting the CF plus a bright probe flash (PF) in tandem, separated by interstimulus intervals (ISIs) of 0.01 to 1.4 seconds, and calculating the proportion of the PF
a
-wave suppressed by the CF at each ISI. To test if similar kinetics describe deactivation, difference of exponential (DoE) functions with common
α
and
t
eff
parameters, respective rate constants for the initiation (
I
) and quenching (
Q
) phases of the response, and specified values of
s
(
s
I
,
s
Q
), were compared to the photoresponse time course.
Results
As hypothesized, the optimal values of
s
I
and
s
Q
were 3 and 2, respectively. Mean ± SD
α
was 0.80 ± 0.066,
I
was 7700 ± 2400 m
2
·cd
–1
·s
–3
, and
Q
was 1.4 ± 0.47 s
–1
. Overall,
r
2
was 0.93.
Conclusions
A method, including a DoE model with just three free parameters (
α
,
I
,
Q
), that robustly captures the magnitude and time-constants of the complete rod response, was produced. Only two steps integrate to quench the rod photoresponse.