Neil Immerman's famous Picture of The World is the following (click to enlarge):
His "Truly feasible" class includes no other class; my question is then:
What is an AC0 problem which is considered to be unpractical, and why?
Neil Immerman's famous Picture of The World is the following (click to enlarge):
His "Truly feasible" class includes no other class; my question is then:
What is an AC0 problem which is considered to be unpractical, and why?
If you want an example of an AC0 function that requires depth $d$, and cannot be computed by AC0 circuits of depth $d-1$, then try the Sipser functions $S^{d,n}$. The superscript $d$ is depth needed for a polynomial-size AC0 circuit. With depth $d-1$, the circuit would need exponentially many gates.
So computing $S^{d,n}$ for $d = 10^{10^{100}}$ would not be "truly feasible."
EDIT: Your question also asks why this would not be feasible. I guess the reason is that $10^{10^{100}}$ is more than the number of atoms in the visible universe.
All this hierarchy is intentionally robust under polynomial changes of the input size. Any class in it can thus contains functions whose complexity is say n^{1000000000} which would be theoretically "feasible" but certainly not practically so. These, however will most likely be very artificial problems. In particular by a counting argument there exists a family of DNF formula (=AC^0 depth 2 circuits) of size n^1000000 which no algorithm whose running time is less than n^999999 can compute. (In a uniform setting we expect something similar but can't prove it.)
The halting problem when the input is represented in unary is in AC^0 and yet quite unfeasible in reality. I'm not sure this is what you meant, but it could be what Immerman meant.