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-, Ek (1,2 ) + ε k̄ = E k̄ (1,2 ) + εk, which highlight the symmetry between the signal and the idler modes.
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-, Ek (1,2 ) + ε k̄ = E k̄ (1,2 ) + εk, which highlight the symmetry between the signal and the idler modes.
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Note that the positions of the signal and the idler modes slightly change for increasing densities as a consequence of the interaction-induced blueshift of the dispersion.
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Note that the positions of the signal and the idler modes slightly change for increasing densities as a consequence of the interaction-induced blueshift of the dispersion.
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40
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It is interesting to note that in the standard Bogolubov theory of equilibrium systems the ungapped, sonic behavior of the Bogolubov dispersion leads to a power-law decay of correlations at T=0.
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It is interesting to note that in the standard Bogolubov theory of equilibrium systems the ungapped, sonic behavior of the Bogolubov dispersion leads to a power-law decay of correlations at T = 0.
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