It is of interest to examine spread function in parallel in both the space and spatial frequency domains. Because all functions to be considered are circularly symmetrical, transformation into the spatial frequency domain involves not the cosine but the Hankel transform, wherein the kernel function is the Bessel function of zero order. In symbols, if the spread function in the object or image plane is defined by
G(
r)
, r = , its representation in the domain of
s, the spatial frequencies, is
where the constant 60 is predicated on the units being used: light spread in minutes of arc visual angles; spatial frequencies in cycles/° of visual angle. In general, image degradation is reflected in a high-spatial frequency deficit. In a thorough analysis of spatial visual processing one tries to disambiguate the contributions of component factors of optical spread, receptor compartmentalization, center/surround retinal neural processing, and so on. Being measured in units of retinal distance, their role becomes increasingly more significant as target size is reduced. That makes the essential difference between traditional visual acuity determination and the approach adopted here so important: target size is unchanged; rather, processing and filtering is confined to the low spatial-frequency region and hence the size relationship between target features, retinal structure, and the intrinsic optical spread of the particular eye remains invariant throughout the process of measurement. It is in this connection that defocus blur needs special consideration. Defocused optical transfer functions are difficult to calculate but fortunately it has been estimated that the error in a geometrical optical over the full diffraction formulation is only about 10% (Hopkins,
1955). It follows that to a good approximation the retinal point spread function for a typical eye with pupil diameter
a and focus error Δ
F is a top-hat function with diameter
aΔ
F radians visual angle. Conversion to visual angle in arcmins, focus error Δ
F of 1 diopters, and pupil diameter
a of 3 mm yields a top-hat retinal point spread of 10 arcmins. Obviously, even neglecting aberrations and a possible influence of the Stiles-Crawford effect, defocus in diopters is not a unique measure of image degradation. An additional aspect of the situation emerges on transfer into the spatial frequency domain: High spatial-frequency components are never completely eliminated by defocus but are merely attenuated and may be subject to phase inversion, and thus occasionally emerge in
spurious resolution, when a high spatial-frequency grating might suddenly appear as resolved in a field otherwise destitute of detail.