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Digital Processing of Quantum-Limited
Images
Conjecture on the Relationship
between Spatial and Temporal Visual Processes
Why do Stabilized Images
Disappear?
A Simple Model for Filling-In,
Contrast, Contrast Constancy and Assimilation
What is “True Color”?
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There are many striking similarities between spatial
and temporal phenomena in vision. For example, the spatial and temporal
contrast sensitivity curves have very similar shapes and both change
in the same way with mean luminance. The relationships between threshold
luminance and stimulus size (Ricco's Law) and threshold luminance
and stimulus duration (Bloch's Law) bear a striking resemblance
over many changes in conditions.
Here is a conjecture: Given any model that explains
a phenomenon related to spatia-1 interactions, the same model will
also explain the related set of temporal phenomena if only one modification
is made to the spatial model, namely that the fact that signals
in neural substrates must travel with finite velocities is taken
into account.
This works for the lateral inhibition model for the
spatial CSF. Make a model in which each input pixel spreads its
signals in an excitatory way over its near neighbors (or maybe only
itself) and in an inhibitory way over cells farther way, the farther
the weaker the interaction. This will yield a band-pass CSF. Then
add to the model the feature that these spreading signals travel
at some finite velocity and so arrive later at farther points, and
a band-pass shaped temporal CSF will result.
This also works for the Intensity-Dependent Spread
model that Jack Yellott and I published. Steve Reuman, in his dissertation
at UC Irvine, showed that the temporal CSF becomes band-pass, that
Bloch's Law follows from Ricco's Law, and also a number of other
interesting relationships. It is also clear that after images, both
positive and negative, will necessarily result if spatial spreading
of signals takes time. (No other assumptions are needed at all to
get after-images, although very likely more are actually needed
to provide a full explanation of real after-images.)
I think I can prove that this conjecture is true
for any linear system, although I don't have the time to do it right.
The conjecture does hold for Intensity-Dependent Spread, which is
fundamentally non-linear, but I don't know how to prove it for non-linear
systems in general. Maybe you do.
Note: (Dennis Baylor showed that the temporal CSF
for a single cone isolated from all interactions with neighbors,
has a band-pass shape, so it cannot be claimed that finite propagation
velocity is the entire explanation for its shape.)
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