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- From: bhv@areaplg2.corp.mot.com (Bronis Vidugiris)
- Subject: Re: Why are elementary particles small?
- Organization: Motorola, CCR&D, CORP, Schaumburg, IL
- Date: Wed, 6 Jan 1993 10:49:04 GMT
- Message-ID: <1993Jan6.104904.11545@lmpsbbs.comm.mot.com>
- References: <1993Jan3.235010.17976@math.ucla.edu> <1993Jan4.022335.25485@news.media.mit.edu> <MATT.93Jan3200346@physics2.berkeley.edu>
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- In article <MATT.93Jan3200346@physics2.berkeley.edu> matt@physics.berkeley.edu writes:
-
- )This is, unfortunately, a confusion of two different senses of what
- )"the size of a particle" means.
- )
- )The first is: quantum-mechanically, we can describe the position of a
- )particle by a wave function. We could, then, say that the size of the
- )particle is the size of the wave packet that describes its position.
- )
- )The second meaning is a somewhat more intrinsic one: when we write a
- )wave function for a particle, are we writing about the spatial
- )distribution of a point object, or an extended object? One way to
- )understand this distinction is to think about interactions; an
- )interaction between point particles is local, but an interaction
- )between extended objects (e.g., protons) involves points separated by
- )spacelike intervals.
- )
- )When particle physicists talk about the sizes of particles, they
- )usually have the second idea in mind, just because it is more
- )intrinsic; after all, you can write an arbitrarily large wave packet
- )for any particle.
- )
- )And as far as we can tell today, photons do appear to be point
- )particles. (As do the other gauge bosons, the gluon, W, and Z.)
-
- A few related points on the 'size' of photon wavepackets.
-
- In 'Quantum Reality', Nick Herbert points out that the 'size' and 'shape' of
- the wavepackets of photons from distant stars is a thin 'fuzzy' disk
- which varies from a *minimum* of about 3ft (don't recall the exact figure) in
- diameter to a maximum larger than the entire solar system. This 'size' can
- actually be experimentally measured using the idea of a 'self-interference
- distance'. Herbert cites "The Intensity Interferometer", Robert Hanbury
- Brown, New York: Halstead Press (1974) for a more complete reference.
- Several stars were actually measured with this device in order to determine
- their angular size (and hence their physical diameter, given that the
- distance to the star can be determined by parallax measurements or other
- means). 'Sizes' up to a limit of several hundred feet (the diameter of the
- apparatus) were actually measured.
-
- If photons from a distant star can be thought of as 'fuzzy disks',
- spectrally pure photons from a laser can be thought of as long fairly
- thin lines. This again comes from a 'self-interference' concept - the
- self-coherent length of a laser is a useful concept when preparing holograms,
- and depends on the spectral purity of the source. I believe that there
- is a limit on the spectral purity of a laser set by the length of its
- resonant cavity - the 'long photon' has to fit inside the resonant cavity
- of the laser, so you can't get a self-coherent length longer than the
- resonant cavity size. [This also suggests that if you 'cut' the 'long'
- photons somehow, say an apparatus which confines the photon to a length
- shorter than its previous self-coherent length, you also destroy the
- spectral purity of the photon/beam. I believe that this would be borne
- out in practice using the Heisenberg principle of measuring location ->
- uncertain angular momentum -> uncertain energy.]
-
- Thus the 'size' of a photon defined in this way isn't really a property
- of the photon itself, or its energy, but of the details of how it is
- 'prepared'.
-
- The ideas of self interference are really more suited to a beam than a
- particle, IMO, and more readily understood in that context. However,
- the idea that light is a particle as well as a wave more-or-less forces us to
- view each individual particle as having 'self-interference' length
- property, even if it doesn't make a lot of sense, as these interference
- patterns do not disappear even when only one photon is present in an
- apparatus at a time.
-