
Thing is the acoustic hole comes along because of the behaviour of fluctuations; at low energies this is fine, but at high energies there's no immediate reason to believe that there isn't something influencing the fluctuations (indeed, there will be) that changes their behaviour enough that now they don't look like they act on a Schwarzschild spacetime. I'd not be surprised to find that you can't write an effective spacetime at all for the high-energy general case, and only at low energies.
The self-interaction term is just coming from a Taylor expansion of the Gibbs free energy. Or it may be the Helmholtz free energy. One of the two. It's also actually not quite a Schroedinger equation because that psi isn't a wavefunction so much as the product of the individual wavefunctions of the atoms in the condensate. So if you follow the kind of arguments made for the low-energy case and put it at high energies you could doubtless write a modification to the Dirac Lagrangian that included an interaction. Just that it would be a bit odd to consider a high-energy Bose-Einstein condensate...
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Tue 8 Dec 2009, 21:38,
archived)
The self-interaction term is just coming from a Taylor expansion of the Gibbs free energy. Or it may be the Helmholtz free energy. One of the two. It's also actually not quite a Schroedinger equation because that psi isn't a wavefunction so much as the product of the individual wavefunctions of the atoms in the condensate. So if you follow the kind of arguments made for the low-energy case and put it at high energies you could doubtless write a modification to the Dirac Lagrangian that included an interaction. Just that it would be a bit odd to consider a high-energy Bose-Einstein condensate...

in fact I believe the two are pretty much the same thing. Having said that, the general case is often difficult and not particularly useful. I couldn't honestly tell you if the Dirac equation has any real world applications outside of particle accelerators. It's just, kind of... nice.
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Tue 8 Dec 2009, 21:58,
archived)

lorentz invariance underpins special relativity -- and general, since special relativity is recovered from general in the flat limit. there'll certainly be real-world applications of it; it's the equation governing the behaviour of relativistic electrons, and if it doesn't have some application somewhere in semiconductor physics that has a bearing on modern computers i'd be quite surprised...
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Tue 8 Dec 2009, 22:05,
archived)