| computable = expressible as Int -> Int Hilbert space = set of functions in Real -> Real geometrical & non-computable = Reals determinism = g(x, t_future) fully set by g(x, t_now) and g if you model a geometric, g : Real -> Real with computable, c : Int -> Int then there are gaps at arbitrarily high precisions, say p (eg., p = delta(g, c) at (x, t)) construct a classical system of arbitrarily complexity (eg., 10^BIG interactions), describe each interaction with g. Since 10^BIG are required, "delta(g, c) < BIG" is required in order for the system to remain deterministic (ie., described by g). We can easily find cases where BIG > delta(g, c), so CM would be non-deterministic if g is replaced by c. As for QM, these "gaps" are cause much deeper contradictions with premises of QM. If you replace wavefunctions, g, with computable ones, c then they dont sum to solutions of the wave-eq, so QM fails to be linear (the detla(g,c) are massive because hibert space is infinite-dim). Now it might be that reality is really computable in the sense that there's some c which can replace g, but this would violate the assumptions of physics and has no motivation. Physics might be wrong, but there's no evidence of that. There are also other issues, but these are just two off the top of my head. Refences: Look for physical church-turing, church-turing thesis, non-det and det in chaos theory, non-det in classical mechanics, physical interpretations of the reals -- this will be in postgrad work, it wont be in popsci books. |
Nobody takes "computable approximation to g: R -> R" to mean "a computable function c: R* -> R" where R is the computable reals. There are many mathematical issues with this caused by self-referential programs (realised by Turing himself in "On Computable Numbers"). Typically you would model it as "c: R* x Q -> R*" where Q is a rational describing your desired precision, right?
> Since 10^BIG are required, "delta(g, c) < BIG" is required in order for the system to remain deterministic (ie., described by g).
I'm not sure what you mean by this - the computable approximation "c" is deterministic essentially by definition. If you mean "in order to remain within some bound of g" I can kinda see what you're saying but in that case you can interleave computations with smaller and smaller precisions (the "Q" I mentioned) in order to work around that issue, right? It won't be efficient, but it will certainly be computable.
> Refences: Look for physical church-turing, church-turing thesis, non-det and det in chaos theory, non-det in classical mechanics, physical interpretations of the reals -- this will be in postgrad work, it wont be in popsci books.
Thanks! I don't know much chaos theory, I'll have a look around for a good textbook.
Edit: I just want to say - you have a pretty wild way of writing that makes it hard for me to tell if you're a crank or not. Either way, reading your posts here has given me a ton of food for thought =) what's your background?