The Bactra Review Brainchildren
Dennett talks about patterns in a single instance of a signal; matters are
somewhat different, and actually a bit easier, if one wants to reproduce a
statistical ensemble. In that case, randomness becomes eminently compressible.
(As I've said before, to model coin tossing, toss a coin.) Moreover, there is
a technique for constructing a (computationally and informationally) minimal
model which has as much predictive power as is available to any pattern based
solely on the signal. (There isn't yet a proof that this model is unique, so
Quine is saved for another day.) For the technique of pattern-finding, and
making highly compressed representations of random ensembles, see James
P. Crutchfield, "The
Calculi of Emergence: Computation, Dynamics and Induction," Physica
D 75 (1994): 11--54; for the optimality results, see
James P. Crutchfield and Cosma Rohilla Shalizi, "Thermodynamic
Depth of Causal States: When Paddling around in Occam's Pool Shallowness Is a
Virtue," Physical Review E59 (1999):
275--283. (I warned you there would be
log-rolling and self-promotion.)
Addendum: There is now a proof of uniqueness, up to the way some
cases of measure zero are handled: see Theorem 3 of Cosma Rohilla Shalizi and
James P. Crutchfield, "Computational Mechanics: Pattern and Prediction,
Structure and Simplicity", Journal of Statistical Physics
104 (2001): 817--879, available in PDF here or as cond-mat/9907176. Where this
leaves Quine, or for that matter Dennett, I shan't attempt to say.