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The measurement problem |
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With regard to the problem of making physical sense of the mathematical formalism of quantum mechanics, the physics community appears to be divided into three factions.
- The first advocates agnosticism. It asserts that the quantum world cannot be described; its features are forever beyond our ken. All we can usefully talk about is statistical correlations between measurement outcomes.
- The second faction aspires to describe the quantum world without reference to measurements.
This faction is split into numerous warring sects. Here is how Chris Fuchs describes the situation:
"Go to any meeting devoted to some aspect of the quantum foundations, and it is like being in a holy city in great tumult. You will find all the religions with all their priests pitted in holy war—the Bohmians, the Consistent Historians, the Transactionalists, the Spontaneous Collapseans, the Einselectionists, the Contextual Objectivists, the outright Everettics, and many more beyond that... They all declare to see the light, the ultimate light..."
- The third faction — arguably the majority — is tired of this spectacle and does not care what (if anything) quantum mechanics is trying to tell us about the nature of Nature.
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Wave functions versus propagators |
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At the heart of the quantum formalism is the amplitude (a.k.a. propagator)
< xf , tf | xi , ti > .
In the case of a single particle, xi and xf are points in "ordinary" 3-space. In general, they are points in the system's configuration space, which has as many dimensions as the system has degrees of freedom. (The absolute square of this amplitude, integrated with respect to xf over a region R of the configuration space, gives the conditional probability of finding the system in R if the appropriate measurement is made at the time tf, the condition being that the particle was last "seen" at xi at the time ti.)
It is customary to introduce the so-called "wave function" Ψ(x,t) by requiring that it satisfy the equation
Ψ(xf,tf) = ∫ dxi < xf , tf | xi , ti > Ψ(xi,ti) .
Wave functions and propagators provide the same information. Knowing either one can calculate the other. Yet some proposed quantum ontologies (most notably, Everett's "many-worlds interpretation") transmogrify the wave function into a representation of "what ultimately exists" and treat the propagator as nothing more than a computational tool.
Whence this partiality? I should have thought that if the propagator is nothing more than a computational tool, then so is the wave function.
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The evolutionary paradigm |
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- Our successive experience of the world's temporal aspect makes it natural for us to hold that only the present is real; the future exists not yet, the past no longer.
- Our self-experience as agents in a successively experienced world makes it natural for us to hold that the past, being known or knowable in principle, is "fixed and settled," that the unknown and apparently unknowable future is "open," and that the open future is determined by the settled past.
If we want to make sense of the physical world, we need to realize that the origin of these notions is psychological — they concern our way of experiencing the world rather than the world itself.
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Time-symmetric probabilities |
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It is obvious why we are more interested in assigning probabilities to later outcomes on the basis of earlier outcomes than in assigning probabilities to earlier outcomes on the basis of later outcomes, but quantum mechanics allows us to do both. It is indifferent to our preference for predictions over retrodictions. It even allows us to assign probabilities on the basis of both earlier and later outcomes, with intriguing consequences.
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The mother of all pseudoproblems |
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An algorithm that serves to assign probabilities to possible measurement outcomes on the basis of actual outcomes has two perfectly normal dependences:
- It depends continuously on the time of measurement: if you change the time of measurement by a small amount, the probabilities assigned to the possible outcomes change by small amounts.
- And it depends discontinuously on the outcomes that constitute the assignment basis: if you take into account an outcome that you did not previously take into account, the assignment basis changes unpredictably as a matter of course, and so do the assigned probabilities.
Misinterpret the algorithm's dependence on the time of measurement as the time dependence of an evolving state of affairs of some kind, and you have to explain why
- at the time of a measurement this state of affairs changes (or appears to change) discontinuously and unpredictably, whereas
- between measurements it evolves continuously and predictably.
As far as physics is concerned, this is the mother of all pseudo-problems.
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The cookie cutter paradigm |
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Most of the time we think and behave as if the visual world — the world as we see it — were a more or less faithful reproduction of the real world "out there," if at all we make the distinction. Apart from the many well-known philosophical objections to this naive attitude, psychological and neurobiological studies in the 1980s and 1990s have uncovered a radically different story: the visual world is a creation (by the mind and/or brain) that is guided by a surprisingly sparse stream of clues from "outside." The way in which this world is created conforms to the cookie cutter paradigm (CCP). It is therefore only natural that we should try to construct our model of the physical world along lines laid down by the CCP, and that we should be perplexed beyond measure by Nature's refusal to follow suit.
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A ta(b)le of two worlds |
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The following table highlights some of the differences between the world according to quantum mechanics (QM) and a world that is constructed along the lines laid down by the CCP. You may smile or scoff at the naivety of some or even most of the items in the second column, which aren't even mutually consistent. (For example, the notion that the ultimate constituents of matter are pointlike objects is at odds with the view that forms are bounding surfaces). All the same, at least some of the items in this column are all but universally accepted, for instance the representation of physical space as an intrinsically and completely differentiated "manifold."
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How are "spooky actions at a distance" possible? |
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Recall those "spooky actions at a distance": Bell's theorem, the experiment of Greenberger, Horne, and Zeilinger, and a follow-up. What is so unsettling is not that we cannot explain them.
As we have seen, no fundamental theory can be explained by a "more fundamental" theory; if there is a "more fundamental" theory, then the "less fundamental" theory isn't fundamental at all. Nor does the classical sleight-of-hand, which consists in the transmogrification of a mathematical algorithm into a physical mechanism or process, produce anything but nonsense.
What is so unsettling is that these spooky actions at a distance do not seem possible at all.
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