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For the low-density limit, we have simply fitted the frequency and phase of our oscillating term to a model pair-distribution function built from Gaussian orbitals centered on the sites of a triangular lattice. In the present work we are dealing with the fluid state, not with the crystal, and the damping of the oscillations is completely different in the two cases. But the position of the maxima, which is practically the same in the fluid and crystalline state, is the only information which we extract from this model.
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