The reaction time (RT) vs spatial frequency (SF) curve is determined,
using gratings from 1 to 40 c/deg, at seven different contrast levels
between 0.95 and 0.02. The form of the RT/SF function: (a) replicated
the inverse of the contrast sensitivity function (CSF) at near thresho
ld contrast levels; (b) behaved differently at higher contrasts, exhib
iting two branches at contrast close to 1. The interpretation is that
there are two factors determining this function: (1) the transition fr
om the operation of fast transient channels at low SF to the operation
of slow sustained channels at high SF, the transition taking place wi
thin a narrow SF band close to 6 or 8 c/deg (depending on the subject)
and (2) the contrast attenuation by the optical and neural transfer f
unction, operating throughout the SF range. At high contrasts, the eff
ect of the first factor can be clearly observed, because the effect of
the second factor does not change with spatial frequency except in a
region where the RT/SF function changes rapidly. At lower contrasts, h
owever, the second factor becomes increasingly relevant while the firs
t becomes less and less observable.