But when r is restricted to the integers, the dynamical system is not chaotic, as there are no periodic orbits and periodic orbits are an essential element of chaos.
That is an excellent repetition of your claim, it doesn't seem like you've included any new content. The definition that I've been using insofar as evolution is concerned is exponential error growth. Restricting to periodic orbits necessarily excludes numerous systems that need to be part of the evolution discussion. For example, the pool(snooker) balls, would be chaotic in the sense of exponential error growth, but not in the sense that they ever have periodic orbits. Moreover, if we use your definition, then it is guaranteed that evolution has nothing to do with chaos, as evolution doesn't have periodic orbits. So the definition you've provided, while perhaps useful in limiting certain mathematical investigations, is self-defeating when applied to the topic at hand, whereas exponential error growth is a perfectly sufficient definition. Why should we restrict chaotic systems to periodic orbits? Is there any reasoning behind this claim?
As far as I have read in textbooks about chaos, chaotic maps are maps of sets in to themselves.
Okay, if that is the constraint you are placing, then closure under the integers was sufficient in the first place.
Outside of some bounded interval ([0,1] in the case of the logistic, any intial interval will eventually not map into itself.
You're wrong. r = .1, x = 10, will map into itself an infinite number of times, on the bounded region [-10,10], although this particular solution will not be chaotic. There actually is a set of solutions that have this property. r = .01, x = 100 [-100,100] r = .001,x = 1000,[-1000,1000] so, technically, there are an infinite number of bounded solutions outside of the interval [0,1] that map onto themselves indefinitely yet do not converge to 0(or ever enter the region [0,1])
Also I've already mentioned this but you seem to have missed it, if we're working with a finite set of integers or we do a normalized plot, it shows just as much chaotic oscillation as any other system. It is just a question of how you visualize the erratic and unpredictable behavior of the output.
Nice assertions. Would you care to back them up with some actual examples?
y = 2*x mod z over the integers is a classical example.(z prime != 2)
Over the rationals: y = 2*x mod 1.0
Both digital and analog systems will make numerical approximations from the mathematical ideal, which has been my contention from the start, and thus they are both equivalent approximations.
ETA: Moreover, if we restrict the discussion to only systems that have dense periodic orbits, it essentially concedes the issue of randomness in evolution. Chaotic systems under your definition are generally subject to noise induced order. This eliminates the possibility of any large scale randomness in evolution.