We do multidimensional deconvolution with causal (one-sided)
one-dimensional filters.
Equation (7) shows such a one-sided filter as
it appears at the end of a 2-D helix.
Figure shows it in three dimensions.
The top plane in Figure
is the 2-D filter seen in equation (7).
The top plane can be visualized as the area around the end of a helix.
Above the top plane are zero-valued anticausal filter coefficients.
3dpef
Figure 13 A 3-D causal filter at the starting end of a 3-D helix. | ![]() |
It is natural to ask,
``why not put the `1' on a corner of the cube?''
We could do that, but that is not the most general possible form.
A special case of Figure ,
stuffing much of the volume with lots of zeros
would amount to a `1' on a corner.
On the other hand, if we assert the basic form has a `1' on a corner
we cannot get Figure
as a special case.
In a later chapter we'll see that we often need as many coefficients
as we can have near the `1'.
In Figure
we lose only those neighboring coefficients
that 1-D causality requires.
Geometrically, the three-dimensional generalization of a helix is like string on a spool, but that analogy does not illuminate our underlying conspiracy, which is to represent multidimensional convolution and deconvolution as one-dimensional.