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Posted: Mon Dec 07, 2009 4:35 pm
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Posted: Mon Dec 07, 2009 4:40 pm
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Posted: Mon Dec 07, 2009 4:48 pm
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Posted: Mon Dec 07, 2009 4:57 pm
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Posted: Mon Dec 07, 2009 5:36 pm
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Posted: Mon Dec 07, 2009 8:30 pm
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Posted: Tue Dec 08, 2009 2:48 am
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Posted: Tue Dec 08, 2009 5:53 pm
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Posted: Tue Dec 08, 2009 8:29 pm
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From the point of view of Fourier analysis, the position-basis and momentum-basis wavefunctions are a Fourier transform pair, whose variances are bounded below by a constant. This is a mathematical fact about Fourier transforms and has no physical content by itself; all the physics is in identifying physical state as a wavefunction in the first place.
More abstractly, quantum observables are operators on a Hilbert space, on which again it is a mathematical theorem that for any state, the expectation values satisfy 4 ≥ |<[A,B]>|², where [A,B] = AB-BA is the commutator. You should be able to find the standard proof using the Cauchy-Schwarz inequality rather easily.
For example, it the position basis, the position operator is just q = x, while the momentum operator is p = -iℏ d/dx. Hence [q,p]f = -iℏ( x(d/dx)f - (d/dx)(xf) ) = -iℏ[ xf' - (f + xf') ] = iℏf, meaning [q,p] = iℏ. Substituting into the above, ≥ ||²/4 = ℏ²/4, i.e., the product of the variances of the position and momentum measurements is bounded below by ℏ²/4.
And yes, photons are about as quantum as it gets. Layra-chan's point was simply that there's absolutely nothing in the HUP that depends on photons. It's a purely geometric consequence of having non-commuting observables living in a Hilbert space.
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Posted: Sat Dec 12, 2009 9:22 am
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