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In an earlier paper we developed a collective motion description of atomic liquids, by expressing the quantum Hamiltonian in terms of rotated components of the density Fourier transform, which allowed the treatment of potential interaction terms without approximations. In the present paper, we further explore the physical content of our formalism and we show how it can be used for calculations in a real system.
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Antoniou et al. (2001) studied this question.
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