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- From: jbaez@riesz.mit.edu (John C. Baez)
- Newsgroups: sci.physics
- Subject: Re: Uncertainty Principle [T.Bollinger => LONG]
- Message-ID: <1992Sep5.170329.9152@galois.mit.edu>
- Date: 5 Sep 92 17:03:29 GMT
- References: <1992Sep4.170847.235@prim> <1992Sep5.071519.16554@asl.dl.nec.com>
- Sender: news@galois.mit.edu
- Organization: MIT Department of Mathematics, Cambridge, MA
- Lines: 112
- Nntp-Posting-Host: riesz
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- In article <1992Sep5.071519.16554@asl.dl.nec.com> terry@aslws01.asl.dl.nec.com (Terry Bollinger) writes:
-
- >THE "DISTURBED PARTICLE" INTERPRETATION OF QUANTUM UNCERTAINTY
-
- >Historically, some of the earlier books on QM certainly tended to describe
- >it that way, especially when folks with an essentially classical background
- >were trying to come to grips with it. But it has problems, and does in fact
- >tend to "overtrivialize" the profoundly bizarre underlying principles that
- >are involved in QM. E.g., Dr. Richard Feynman found such views misleading
- >and somewhat offensive, and in his writings he argues against relying too
- >heavily on such analogies.
-
- I have often wondered about the fact that the Gedankenexperimenten used
- to argue for the uncertainty principle in the first place are based on
- what seems like classical reasoning TOGETHER with the assumption E =
- hbar nu relating the energy and frequency of a photon, or p =
- hbar/lambda relating the momentum and wavelength. These arguments tend
- to work along the lines that to see something you have to hit it with
- photons, and to see it accurately you have to use photons of short
- wavelength hence lots of energy and momentum, which disturb what you're
- trying to see. What do these arguments really prove, if anything? Of
- course, historically they they were used to arrive at the current
- framework of quantum mechanics and one can feel free to forget them once
- you buy this framework. But it still is interesting to ponder how these
- arguments manage to convince people of the necessity of the uncertainty
- principle. Certainly you can't prove by pure logic that the world must
- be quantum mechanical rather than classical! These arguments seem to be
- using the properties of photons to "sneak quantum mechanics in the back
- door". Perhaps they are showing that a world with light described
- quantum-mechanically and other particles described classically is
- inconsistent or otherwise incoherent? It would be nice if someone could
- extract the rigorous core, if any, out of these hand-wavy arguments.
-
- >In Vol. III of his Lectures he goes to some
- >lengths to point out that in Stern-Gerlaugh the separation of the base
- >states does *not* "disturb" the particles in the sense of irreversibly
- >preventing the original composite state from being recovered. You can
- >"rebuild" the state simply by recombining the base state paths -- something
- >that makes no sense at all from a strict disturb-the-states perspective.
-
- If you look at my explanation of your angular momentum puzzle -
- which seems essentially the same as Mcirvin's - you will see that it
- relies on the fact that measuring one component of the angular momentum
- of a particle really does affect other components of the angular
- momentum of the particle. (I made this precise in my previous post.
- Basically, all I mean is that if you measure J_x of an electron, then
- J_y, then J_x, you needn't get the same answer for J_x both times; in my
- previous post I said how to reconcile this with conservation of angular
- momentum.) So unless this is full of baloney, there DOES seem to be
- something to the "disturb-the-particle" view of uncertainty - although
- it doesn't tell the whole story.
-
- It's rather murky to me right now.
-
- >THE FOURIER TRANSFORM INTERPRETATION OF QUANTUM UNCERTAINTY
- >
- >One of the most beautiful and readable discussions I've seen on this subject
- >is by Dr. Roger Penrose in his popular book "The Emperor's New Mind." On
- >pages 243-250 of the paperback edition you will find two sections entitled
- >"The quantum state of a particle" and "The uncertainty principle." What
- >you will read is a fascinating discussion of the remarkable symmetry that
- >lies between particles as they are described in "ordinary" space of three
- >dimensions, and "momentum" space in which they are positions according to
- >their momentum values instead of their ordinary-space locations.
-
- >In Dr. Penrose's discussion, the wavefunction that describes a particle
- >has the appearance of a corkscrew in both of these spaces.
-
- To the mathematically literate a formula for the wavefunction might
- clarify these mysterious corkscrews a lot. The lay audience could
- easily be forgiven for thinking that quantum corkscrews are just as
- screwy as space potatos. I am trying to think of a function from the
- real numbers to the complex numbers whose graph looks like a corkscrew,
- AS DOES that of its Fourier transform. I guess a Gaussian times a
- complex exponential does the trick:
-
- exp(ikx - (x-a)^2/c^2)
-
- will be a Gaussian bump of width c centered at a times a complex
- exponential (a "corkscrew") of frequency k. The Fourier transform of
- such a function will be another of the same general form (times some
- constant). These functions are especially nice when studying position
- and momentum operators, Fourier transforms and such; a real workout on
- their mathematical structure can be found in Folland's book Harmonic
- Analysis on Phase Space.
-
- >The resulting relationships are like some sort of pair of clubs with a long-
- >term unresolved dispute about joint membership. Join one of the clubs 100%
- >(make your corkscrew so short that you have an EXACT location in either
- >ordinary space or momentum space), and you are 100% LOST from the other
- >club. Your location in it becomes scattered literally over the entire
- >universe, so that at any one location you're probability of being "found"
- >by a detector becomes flat-out zero. A distressing state of affairs!
-
- I sorta like it myself. For many beautiful theorems quantifying exactly
- how a wavefunction that is concentrated in position space has to be
- spread out in momentum space, check out Folland's book. Gaussians are
- the functions that come the closest to being members of both clubs.
-
-
- >HIDDEN VARIABLES, PILOT WAVES, AND THE DANGERS OF PHILOSOPHICAL EXTREMES
-
- >BTW, it's my guess that part of the reason of the reason why Dr. David Bohm,
- >author of a superb text on QM and a neo-hidden-variable "pilot wave" in his
- >interpretation of QM, unexpectely went New-Agey on everbody.
-
- A rather odd sentence, that, but I get your drift. :-) Another victim
- of the lure of quantum quackery (in my humble opinion) is Josephson, the
- Nobelist of "Josephson junction" fame - whose circuits use sneaky
- quantum tricks closely related to the Bohm-Aharanov effect. Check out
- his letter to the editor in the August (?) "Physics Today" in which he
- defends Jahn's research on telekinesis!
-