I Finite universe, quantized linear momentum, and the HUP....

asimov42
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Hi all,

Yet another question: if the universe is finite, then linear momentum should be quantized (I assume in a similar manner to an infinite potential well since there are boundary conditions). My question is, then, if one computes a value for ##\Delta p## (momentum variance), is the variance also quantized? Due to the uncertainty principle, the variance cannot be zero - but I'm unsure about the implications of quantized momentum.
 
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The variance is not quantized. The variance comes from superposition principle, and coefficients of superposition can take any values (constrained only by the overall normalization condition).
 
So there would be a finite number of momentum states, but the probability distribution over superpositions of those states (combinations) is continuous, hence continuous values for variance?
 
There is no quantized momentum in a finite universe.
 
Is it not the case that momentum would have to be quantized? Since the universe has finite size, don't the boundary conditions enforce quantization (albeit with extremely small separation for a universe of any reasonable size).
 
asimov42 said:
Is it not the case that momentum would have to be quantized? Since the universe has finite size, don't the boundary conditions enforce quantization (albeit with extremely small separation for a universe of any reasonable size).

If the Universe has a boundary, there is no momentum operator whose eigenvalues can be quantised. The presence of the boundary breaks translational invariance.

You might consider a compact universe (such as considering a particle living on a circle) where something like momentum exists (actually, more like angular momentum, but let's skip that for now).
 
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Thanks @Orodruin! Are there implications then for a universe with a boundary? If translational invariance is broken (something I hadn't thought about), then this also break momentum conservation (at the boundary), correct? Presumably this does not have implications for the uncertainty principle?
 
asimov42 said:
Are there implications then for a universe with a boundary? If translational invariance is broken (something I hadn't thought about), then this also break momentum conservation (at the boundary), correct? Presumably this does not have implications for the uncertainty principle?

Also, with a boundary in place, the wavefunction would not be differentiable at the boundary itself - how is this dealt with? (since both the wavefunction and its derivative should be continuous)
 
asimov42 said:
Also, with a boundary in place, the wavefunction would not be differentiable at the boundary itself - how is this dealt with? (since both the wavefunction and its derivative should be continuous)
It is differentiable and continuous. If you are thinking "wave function = 0" outside: It is not. The outside is not part of the domain of the wave function.

Also, the "continuous and differentiable" is a truth with modification that makes some assumptions about the potential. Consider what happens in a delta function potential.
 
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Ah I see - what about at the exact boundary itself? (this would be the set of all points that actually are 'on' the boundary, if one can specify such a thing) If I understand correctly, you're saying there is no discontinuity in the derivative because all points are 'inside' the universe? So the analogy of an infinite square well isn't really correct.
 
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asimov42 said:
So there would be a finite number of momentum states, but the probability distribution over superpositions of those states (combinations) is continuous, hence continuous values for variance?
Yes.
 

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