The densities of photoreceptors and ganglion cells changes substantially even within the fovea. The models of neural contrast sensitivity agreed quite well (
Figure 6) with literature that used many different sized targets, despite the fact that those stimuli would have fallen over retinal areas with different sampling densities (and therefore different spatial frequency sensitivity curves). Nonetheless, the models of neural contrast sensitivity utilized by the present modeling could practically be considered unaffected by Piper's law—that is, being measured using a stimulus of sufficient extent (sufficient number of cycles) so as to be independent of stimulus area. We feel this to be a reasonable assumption given that the data of Xu et al.
(2017) were made to agree with those of Campbell and Green
(1965), which were measured using a 30° stimulus; therefore, at least 30 cycles were visible for all spatial frequencies tested. Literature has shown that spatial summation and, by extension, contrast sensitivity suffer when fewer than approximately eight (
Robson & Graham, 1981) or ten (
Howell & Hess, 1978) cycles are visible. Therefore, the modeling may not be representative of tasks that involve very small targets where spatial details are insufficiently represented. Similarly, Hoekstra, van der Goot, van den Brink, and Bilsen
(1974) found that the critical number of cycles varied with target luminance, but they found that the critical number of cycles decreased (fewer visible cycles were necessary) with decreasing luminance. At all of the luminances tested by Hoekstra et al.
(1974) (ranging from 2 to 600 cd/m
2), the critical number of cycles appeared (from their Figure 1) to occur at fewer than 10 cycles.