Dave Krantz on decision analysis and quantum physics, leading to a Jim Thomspon reference and then back to Penrose’s theory that consciousness is inherently quantum-mechanical

Commenting on my thoughts about decision analysis and Schroedinger’s cat (see here for my clarifications), Dave Krantz writes,

I’d first like to comment on the cat example, and then turn to the relationship to probabilistic modelling of choice.

I think one can gain clarity by thinking about simpler analogs to Schroedinger’s cat. Instead of poison gas being released, killing the cat, let’s suppose that a single radioactive decay just releases one molecule of hydrogen (H2) into an otherwise empty (hard vacuum) cat box. Now an H2 molecule is something that, in principle, one can describe pretty well by a rather complicated wave function. The wave function for an H2 molecule confined to a small volume, however, is different from the wave function for an H2 molecule confined to a much larger cat box. At any point in time, our best description (vis-a-vis potential measurements we could make that would interact with the H2 molecule) is a superposition of these two wave functions, narrowly or broadly confined. As long as we don’t know whether the radioactive decay has taken place, and we make no observation that directly or indirectly interacts with the H2 molecule, the superposition continues to be the best physical model.

This example points up the fact that Schroedinger’s cat involves two different puzzles. The first is epistemological: we are used to thinking of a cat as alive or dead, but equally used to thinking of a H2 molecule as confined narrowly or broadly. How can it be both? But this way of thinking just won’t work in QM. The point of the double-slit experiments is to show clearly that an unobserved photon does NOT go through one slit or the other, it goes through both, in the sense of its wave function giving rise to coherent circularly symmetric waves emanating from each slit and interfering. It is equally wrong to think that a H2 molecule is either confined narrowly or broadly. Observations are going to be accounted for by assuming a superposition.

The second puzzle arises because a cat cannot in practice be described by a single wave function at all. That’s at least true of an ordinary cat, subject to many sorts of observation. But in practice, even an unobserved cat is not describable by a wave function. There are wave functions for each molecule, but the best descriptions do not collapse these into a single wave function. Coherence fails. To take an analogy, one can get monochromatic light by passing a beam through an interference filter; though the frequencies of the different photons are all alike, the phases still vary randomly. This is very different from the coherent light of a laser, where everything is in phase.

There is a real problem of understanding when incoherent wave functions collapse into a single coherent one. This has been dramatized, in recent years, by studies of Bose-Einstein condensates. Rubidium atoms can be very near one another, yet still incoherent; but at low temperatures, they become a single molecular system, with a condensed wave function. The study of conditions for coherence is on-going, as I understand it. A cat is outside the boundaries of coherence.

Epistemologically, the introduction of probabilities as fundamental terms in choice modelling is rather analogous to the introduction of probabilities in QM measurement. It has always struck me as curious that the two happened in the same year, 1927: Born developed the probabilistic interpretation of QM measurement and Thurstone formulated the law of comparative judgment.

Where the analogy breaks down, however, is that there isn’t any analog to a wave function in choice models. Thurstone actually tried to introduce something like it, with his discriminal processes, but from the start, discriminal processes were postulated to be independent rather than coherent random variables. Thus, I don’t see much point in pushing the analogy of any DM problem with the Schroedinger cat problem, where the essence is superposition rather than independence.

My thoughts

OK, that was Dave talking. To address his last point, yes, I don’t see where the complex wave function would come in. (Dsquared makes the same point in the comments to this entry. In probability theory we’re all happy to use Boltzmann statistics (i.e., classical probability theory). I’ve never seen anyone make a convincing case (or even try to make a case) that, for example, Fermi-Dirac statistics should be used for making business decisions.)

It cannot be denied that making business decisions can often seem overwhelming. Howecademy.co.uk/assertiveness-training/”>click here) to help them develop these skills, giving them much more confidence when making business decisions. However, that being said, I know so many people who like to use an OKR goal-setting approach to combat decision fatigue.

But what is OKR goal-setting? Put simply, objectives (O) are memorable qualitative descriptions of what you want to achieve and key results (KR) are a set of metrics that measure your progress towards the objective. For each objective, you need a set of 2 to 5 key results. You can learn more about OKR software that can boost your decision-making process by visiting Profit.co.

That being said, Dave’s point above about “coherence” is exactly what I was talking about. Also there’s the bit about the collapse of the wave function (or of the decision tree). But I suppose Dave would say that, without complex wavefunctions, there’s no paradox there. With classical Boltzmann statistics, the cat really is just alive or dead all along, with no need for superposition of states.

Jim Thompson’s cat

Hmmm…my feeling is that the act of deliberation, or even just of keeping a decision “open” or “alive,” creates a superposition of states. If I’m deciding whether or not to flip the switch, then I would’t say that the cat is “either alive or dead.” I haven’t decided yet! In The Killer Inside Me, Jim Thompson writes, “How can you hurt someone that’s already dead?”, but I don’t take such a fatalistic position.

Roger Penrose’s consciousness

But hey, let’s take this one step further. In my experiment (as opposed to Schroedinger’s), the cat is alive or dead based on my decision of whether to flip a switch (and, in turn, this decision is ultimately coupled with other outcomes of interest; e.g., the switch also turns off the light in the next room, which encourages the lab assistant to go home for the day, and then he might bump into someone on the subway, etc., etc.). If it is true, as Penrose claims in The Emperor’s New Mind, that consciousness is inherently quantum-mechanical and non-algorithmic, then my decision of whether to flip the switch indeed must be modeled as a superposition of wave functions. Although then I’m not quite sure how deliberation fits in to all this.

Anyway, to get more positivistic for a moment, maybe the next research step is to formulate some actual decision problems (or realistic-seeming fake problems) in terms of coherence, and see if anything useful comes of it.

P.S. Dave is very modest on his webpage but he’s actually the deepest thinker I know of in decision analysis.

P.P.S. It’s funny that Dave has a cat living in a “cat box,” which I always thought was equivalent to the litterbox (so I recall from my catful days). Maybe “cat container” would be a better phrase?

5 thoughts on “Dave Krantz on decision analysis and quantum physics, leading to a Jim Thomspon reference and then back to Penrose’s theory that consciousness is inherently quantum-mechanical

  1. Dave Krantz: Where the analogy breaks down, however, is that there isn't any analog to a wave function in choice models. Thurstone actually tried to introduce something like it, with his discriminal processes, but from the start, discriminal processes were postulated to be independent rather than coherent random variables. Thus, I don't see much point in pushing the analogy of any DM problem with the Schroedinger cat problem, where the essence is superposition rather than independence.

    I proposed one interesting aspect of the QM/DM analogy and Andrew proposed two. Dave says he doesn't see any analogy.

    Yet Andrew sees Dave as "the deepest thinker I know of in decision analysis."

    So are you saying that he is right and we are wrong and there are no interesting analogies between quantum mechanics and decision making?

    More generally, what exactly is it in Dave's quote that you find insightful and deep? I did not learn anything new about the relationship between QM and DM from it?

  2. There might be some play in identifying the complex part of a quantum probability with "weight" in the Keynesian sense because Keynes' weight certainly has a connection to the extent to which one is prepared to regard a probability judgement as actionable; I don't know enough about Keynesian probability to say any more about this though.

  3. Deb,

    My impressions of Dave come from hundreds of conversations. I found all of his message on this topic to be interesting, although my own thoughts in this area are still too confused to identify exactly what parts will be useful.

    Dsquared,

    I've only encountered Kaynes's probability theory through secondary sources but I don't recall the "entanglement" issue arising.

  4. You state: "I've never seen anyone make a convincing case (or even try to make a case) that, for example, Fermi-Dirac statistics should be used for making business decisions."

    Well I have (sort of). I ran accross the example many years ago. The example occured in a book on applications of Maximum Entropy. (Both Fermi-Dirac and Bose-Einstein statistics can be viewed as MaxEnt distributions).

    The specific application of MaxEnt I saw in the book was an inventory control problem. In the problem the i'th "state" had at most N_i "elements". The end result of the problem was that you get a family of maxent distributions (that can be worked out analytically) that was charaterised by the N_i's. The interesting thing was that if you let all the N_i's go to infinity you get the Bose-Einstein distribution. If you set all the N_i's equal to 2 you get Fermi-Dirac statistics.

    Obviously in a real inventory control setting the N_i's are not all going to be equal to 2, but I still think this qualifies as an example of Fermi-Dirac statistics appearing in a business decision setting.

  5. For the vast majority of real life decisions, Pascalian probabilities work just fine. If you really want to quantify second order uncertainty, Glenn Shafer provides a cousin of Pascalian probability which some people refer to to as Baconian probabilities.

    AG suggested that in general, fancy shmancy formalisms designed to model quantum behavior do not apply very often to real life decisions. Some people disagree, arguing that in certain specialized business decisions, Fermi-Dirac probabilities are applicable.

    I do not know what an FD probability is. But I second Andrew's motion that for the vast majority of decisions people encounter in life, Pascalian probabilities work fine. [Although we'd probably be better off if we upgraded to some Shaferian/Baconian representation of uncertainty – it really is useful to track second order uncertainty.]

Comments are closed.