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- From: mcirvin@husc8.harvard.edu (Matt McIrvin)
- Newsgroups: sci.physics
- Subject: Re: What does quantum have to do with it?
- Message-ID: <mcirvin.727991393@husc.harvard.edu>
- Date: 25 Jan 93 19:49:53 GMT
- Article-I.D.: husc.mcirvin.727991393
- References: <1993Jan25.134627.22922@oracorp.com>
- Lines: 71
- Nntp-Posting-Host: husc8.harvard.edu
-
- daryl@oracorp.com (Daryl McCullough) writes:
-
- >Maybe the situation is analogous to using coordinates to describe
- >locations in space. The coordinate description gives a special status
- >to this one location, the origin. However, the laws of physics don't
- >really treat the origin any different from any other point. Maybe
- >measurement is in the same position; Quantum mechanics doesn't really
- >treat measurement devices any different, but nevertheless it is
- >necessary to decide what are the measurement devices.
-
- This is not a bad description of the sort of interpretation John Baez
- talked about a while ago; I suspect that the historic Copenhagenites and
- those who go on about "questions being outside the realm of physics" are
- really thinking about something similar. The idea is that *all* QM
- really predicts are conditional probabilities: the probability of
- B given A. How you set up A and how you find out the system is in B
- are not described within the QM calculation; in that sense
- measurements are treated as special. But measurements are *not* treated
- as special in the sense that you can perform other "measurements" with
- the *same* apparatus in between A and B, and as long as you take everything
- into account, *those* processes are treated in the same way as everything
- else, using quantum mechanics. There's no physical difference between
- the apparatus in its capacity as the maker of observations and the
- apparatus in its capacity as a physical object; the only difference is
- in which calculation you're doing, which question you're trying to
- answer.
-
- Some people have expressed this as "treating the measuring device
- classically" when it's outside the quantum-mechanical evolution in
- the calculation. I think that is misleading if only because many
- measuring devices wouldn't work classically-- suppose it has integrated
- circuits in it! For that matter, if it were really treated classically
- you'd calculate that its atoms would collapse, yielding no measurement
- at all. A better statement is that you don't "treat" the measuring
- device at all in the calculation when it's used to make the
- measurements. Whether the measuring device works or not is a
- different question, one just as accessible to quantum mechanics.
-
- I think this is what Wheeler means when he talks about "the distinction
- between the probe and the probed" as the important thing in QM
- measurement. The distinction is arbitrary, but it's the first thing
- you have to do when finding something out.
-
- When taken to an extreme this becomes a kind of operationalist view:
- physics then concerns itself *only* with predicting laboratory
- probabilities. I have a little of the same problem you do when swallowing
- this kind of operationalism. You gave the example of black-hole
- quantum mechanics; I'm bothered by something comparatively mundane,
- namely particle physics. An *extreme* operationalist might well regard
- particle physics as the science of what detector readings one can expect
- to find when one builds a certain billion-dollar machine and turns it on.
- If this is the case, the whole enterprise seems pointless, since if you
- don't build the machine in the first place, you know all there is to
- know! (I suppose this could be taken as a knockout argument against
- SSC funding. :')
-
- I have a certain need to believe that the repeatability of
- these experiments says *something* about the structure of the world
- "out there." It doesn't have to be anything so concrete as a reification
- of the wave function; I'm imagining something more like a description of
- the world as what you get when you take the predicted results and
- mod out the possible variations in experimental schemes. The physical
- description of the universe would have something to do with the totality
- of probabilities P(b,a), which is expressed independently of the
- experimental setup-- the simplicity of the world would be related to
- the simplicity of relating probabilities to each other.
-
- This very well may be better described as metaphysics than as physics,
- but it's at the very least physically motivated metaphysics.
- --
- Matt McIrvin
-