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Re: Time and change



Hi Pete,
 
Four quick comments:
 
1) "There is no quantum measurement paradox." !!??  So, the impredicativity Rosen described will not stand? I am intrigued - please comment further on this, as this is a distinct topic from the time topic!
 
2) For others who may not be sure what I was referring to, here is the quote regarding "incommensurable timeframes" is as follows:
"In a nutshell, we find that impredicativities (i.e., complexity) and pure syntax are incompatible. More specifically, complexity and an ontology based on a single syntactic time frame (the ordering of purely syntactic operations into individual steps) are incompatible. In the present context, in which we have identified impredicativities with nonfractionabilities, we cannot build nonfractionable systems by purely syntactic means either. We must accordingly either invoke semantic elements transcendental to syntactics (e.g., taking of limits) or (what may be equivalent) utilizing two or more incommensurable time frames." [EL 294-295]
 
Certainly, in this quote Rosen refers to context-dependence, as you pointed out; in this case, that context-dependence comes in the form of nonfractionability that Rosen is discussing. Rosen offers two alternatives: semantic aspects that cannot be reduced to syntax or incommensurable time frames. It is not clear from the discussion whether these are two sides of one coin, or two non-interchangeable strategies.
 
 
3) "Relative complexity" and similar notions that rely on algorithm (or combinations or sums or size of algorithms) all relate to systems that are inherently "simple systems" in Rosenspeak. They are manners of comparing complication, not complexity. In general, I have not found Chaitin's work to be relevant for Rosennean complexity, since Rosennean complex systems are, by their nature, non-algorithmic, and so too would any measure of their complexity not be based in such algorithmic measures. 
 
 
4) Regarding relativity, mutuality and context-dependence.
I do not know what you mean by this middle ground of "mutuality". To me, either a system allows algorithmic translations (relativity) or not (context-dependence). The bifurcation between Rosennean simple systems (which must be context-independent) and complex ones is quite precise in the distinction between algorithmic and non-algorithmic. I can see no middle ground here. Chaitin's work allows such a concept of mutuality because it is all situated within the realm of algorithmic systems, but it is thereby irrelevant for Rosennean complex systems.
 
 
5) I would consider non-integrability, undecidability, incomputability, etc. to be perhaps examples of incommensurability. But I would not say that they are the same as incommensurability.
I take incommensurability as the dictionary indicates: "having no common measure or divisor or standard of comparison".
 
6) More importantly, as I see it, algorithmic independence (as the sum of two other algorithmic complexities) is NOT at all "semantically equivalent" to incommensurability. Alg. indep. refers to comparisons of information content of the smallest program H(x,y) in comparison to the size of smallest programs for H(x) + H(y). Algorithmic independence refers to optimality conditions for computational strategies, not incommensurability. (http://www.cs.umaine.edu/~chaitin/dijon.pdf)
 
 
I look forward to your more complete exposition!
 
Regards,
Tim
 
 
-----Original Message-----
From: ROSEN Forum [mailto:***On Behalf Of Pete Giansante
Sent: Tuesday, October 28, 2003 9:51 AM
To: ***
Subject: Re: Time and change

Hi Tim:

This is a brief interim message, by way of immediate response to your October 27 post (excerpted below), with my preliminary comments interposed in sequence. I intend to reply more fully in my next post, integrating my complete response with the content of my next message. I have identified the "problem" with the way we view time in contemporary physics, and I know the solution-in-principle; now I must figure out how to articulate it in a way that would convince me if I were walking in on this discussion cold, and were just seeing it for the first time.

Tim Gwinn wrote:
Continuing thoughts on time and impredicativity, with note of Judith's 10/26 remarks.
 
First of all, I would be surprised if no one challenged my assertion that the study of time involves the impredicativiy I described.
Well, I intend to reply to your assertion, but I hope you won't be dissapointed if it doesn't show up as a challenge, as much as it does as a clarification. I don't see it as a matter of agreement or disagreement. You're talking about one thing, and you're doing it from a certain perspective that seems to dead-end in an impredicativity. RR has already resolved it, as I will demonstrate. I talked around it in my last post -- not intentionally, but rather because I hadn't thought my way through it yet. It's much clearer to me now.
This impredicativity is something that occurred to me some time ago but which I had kept setting aside because it was personally unsatisfying in the kinds of limits it implied for any study of temporal phenomena.  It may well be that someone will notice that there are observables, or combinations of observables, relevant to time that do not fall within the confines of the impredicative situation and that therefore we have other ways to study time and (more importantly, perhaps) to ask deeper questions about time.
I think you're on the right track here.
 
That being said, if the impredicativity I have described stands, it would hardly be a death-knell to the study of temporal phenomena. As you may recall, the point of departure for Rosen's book "Fundamentals of Measurement" was another impredicativity: the measurement problem in QM. From examination of that problem flowed all the insights and formal representational systems which comprise that book.
I'm at a disadvantage here, because I still haven't succeeded in glomming onto a copy of Fundamentals of Measurement. Nevertheless, I don't think it will matter; the impredicativity does not stand. There is no quantum measurement paradox.
 
Likewise, the impredicativity with regard to time seems to me to offer many avenues for the investigation of time. For one, the question "what is a clock?" spawns an entire field of inquiry. We can ask things like "can the system itself be the clock?" which can lead to Rosen's notion of "age"[AS 4.8]; "Can a system have multiple clocks moving at different rates?" which can lead to anticipatory systems; "Are the units of time (the ticks of the clock) always the same?" shows up in his discussion of Hamiltonian systems[AS 4.5]; and on. Perhaps complex systems may always involve "two or more incommensurable time frames"? [EL 295].
Perhaps... but I don't know whether that's a necessary constraint for all complex systems -- at least with respect to time. Some systems have relative complexity; that is, their relative complexity is the size of the smallest program (algorithm) it takes to calculate the complexity of System A if we already have an algorithm for calculating the complexity of System B. (Yes, that's a big " if ", but Chaitin proved it in 1975 with his decomposition theorem.) [Note: Chaitin doesn't appear to be referring to Rosennean complexity. indeed, in such a  syntactic approach as the one in which he excels, semantic content is low. Nevertheless, there's an important equivalency to other concepts that integrate with RR's work, which concepts I'll illustrate presently.] An entailment of the same theorem is another concept called the mutual complexity of two given systems, which is defined as the extent to which the complexity of the systems is less than the sum of their individual complexities. But there's a third type of complexity called algorithmic independence, in which the total complexity of the pair is equal to the sum of their individual complexities. That would be semantically equivalent to your concept of incommensurability.

Your mention of incommensurability is interesting, but it might be nothing more esoteric than the inclusion of context-dependent system constraints, as distinct from merely relative ones. That was an important distinction that you yourself made in your October 22 post, and I immediately recognized it as a critical distinction. It suggested a particular line of inquiry that put me on the track of the real nature of the problem.

The distinction, of course, is that in the case of relativity, the differences between any two given systems may superficially appear to be great, but in fact they are related in that one is algorithmically convertible to the other. In other words, they have equivalent encodings, in RR-speak. Midway between relativity and context-dependency is the case of mutuality, in which there is a degree of overlapping complexity. Finally, we have the case of context-dependency, in which there is no way to map one system to the other; that is, the systems do not have equivalent encodings, nor can any method be devised whereby the encodings can be equilibrated. That case is the semantic equivalent of your concept of incommensurability.

There is a long history of gradual refinement of the concept of incommensurability. Poincaré called it non-integrability; Godel called it undecidability; Turing called it incomputability; Prigogine called it non-isomorphism; and Chaitin called it algorithmic independence. Same principle... different languages. From my perspective, it's remarkable to find that principle identified in such a broad cross-disciplinary sampling. But even more remarkably, every one of those threads leads me directly back to Rosennean complexity. For me, none of those examples, individually, has sufficiently penetrating semantic content in its original context to imply the sense of integrability that they all have -- in the aggregate -- in context with RR's take on the same principle: RR called it non-equivalent encodings. From my perspective, there's your concept of incommensurability, and I don't believe that it has anything to do with time, in its most fundamental interpretation & manifestation. More on this in a later post.
 
Further, the relation of clocks to morphogenesis in biological systems is similarly then less obvious and deserving of study on its own. Is it sensible to use one common clocktime to describe the various morphogenetic processes (and their relationships) which by outward appearance (i.e., by a common clocktime) seem to be "simultaneous"?
Maybe... that is, it might be sensible for, say, the purpose of fleshing out some of the process details reductionistically; I mean, that kind of work ultimately must be done as a precursor to the development of practical (technological) applications , but it's not apparent to me that such an approach will provide a theoretical description that will have the broadest applicability. I think there's a more fundamental approach for the purpose of creating a useful theoretical model. (Later for this one, too.)

(snip)
P.S. - When I think about "time", one formalism that keeps nagging at me is "projective geometry". I haven't found a way to make use of it......yet. But it keeps coming to mind - particularly, the notion of "homogenous coordinates" which the topic uses. I just thought I'd mention it to see if it triggers something in one of you out there. :)
It triggers my curiosity, but I don't get very far with it... probably due to my own ignorance of the subject. If you're comfortable about indulging your own nagging thoughts (something I would strongly encourage you to do!), I'd be interested in seeing where you go with it. Since you're not claiming to have an integrated theory and it's still in the cooking stage, that sufficiently qualifies it as hypothetical musing, hypothesizing, speculation... or other suitable qualifier. Go for it. It sounds intriguing.

Regards,

Pete
 
 
-----Original Message-----
From: ROSEN Forum [mailto:***]On Behalf Of Tim Gwinn
Sent: Saturday, October 25, 2003 11:08 PM
To: ***
Subject: Re: Time and change

After thinking yet some more about "time", I am inclined to think that the situation we are in with regard to time is somewhat akin to the limitation in physics we know as "the measurement problem" in quantum mechanics.
 
Rosen describes the key aspect of the measurement problem as follows:
"The problem here is that the very acquisition of data, the very cognition of phenomena (phenotype) in a material system, requires one to consider a larger system ("system + observer") and not to consider smaller ones, as reductionism (or context-independence, or objectivity) requires. This in turn creates a chicken-egg situation, an impredicativity; specifically, one must know the larger system to characterize the smaller, but one cannot know  the larger until the smaller is characterized." [EL 106]
 
With time, I feel we are in a similar situation. In this case the "smaller system" is some system which exhibits  the apparent quality of "time" we want to describe using terms like dynamism/change/process/action/etc. But, we cannot know this quality of this smaller system except by considering a larger system, consisting of the ("system + observer + clock-reference-system"). Here the clock-reference-system is some system which acts to generate the time labels or references. This can be an actual clock, or the sun moving across the sky, or even our internal awareness of our changing thoughts (as Mach noted). Without some such reference system we cannot even have a sense of the "passage of time".
 
If this is so, then it seems to me that the scientific investigation of time will be circumscribed by this impredicativity in the same way that scientific investigations of quantum systems are circumscribed by the impredicative nature of the measurement problem. As a result, it seems to me that the dynamical qualities of systems can only be studied with reference to some clock system.  This impredicativity also thereby sets limits on the sensibility of questions about time that are outside of that circumscribed realm. 
 
Note that the clock system need not always be separate from the system itself. In the discussion of "Time and Age" [AS 4.8], Rosen demonstrates that "age" is perhaps most accurately portrayed not by reference to some external common clock time, but by a dimensionless quantity in which the changes in state of the system are themselves the basis for the "units of time" used to detemine the system's "age".  With his example of a system having radioactive decay, he notes "If we measure time in units proportional to the rate of decay (e.g., in half-lives), then all systems obeying [an equation of radioactive decay] decay at the same rate." [AS 273] However, this kind of measure is often unsatisfying for most of our investigations of dynamical qualities: we generally want to contrast their dynamical qualities with those of their environment and/or other particular systems (e.g., ourselves!), and thus we generally invoke some system external to the one under study to act as the clock reference system.
 
Regards,
Tim