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1
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85034870076
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For a review of colloidal systems see:
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42
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85034876093
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For example, all cases considered in Ref. 17 where the finite size of ions is explicitly included (see Ref. 62) are readily mapped into this two-dimensional space.
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43
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85034868288
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While longitudinal phonons of colloidal systems are overdamped by backflow of the fluid, shear modes of small wave vector propagate: see
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44
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0001383459
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As noted in the text, the choice of ballistic or diffusive dynamics does not effect the stable phase. Thus the phonon frequencies calculated are relevant to studies of phase equilibria.
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(1979)
J. Colloid Interface Sci.
, vol.71
, pp. 622
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Joanny, J.F.1
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49
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85034878700
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See, for example
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57
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84950560410
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The leading correction to the [formula omitted] limit of [formula omitted] is of order [formula omitted] and dominates as long as the dispersion relation is nearly linear for k within [formula omitted] of the Brillouin zone boundary. For the bcc structure at [formula omitted] the dispersion remains nonlinear to very small k and convergence is slow. Even for [formula omitted] results for [formula omitted] are not in the asymptotic limit. This unusual behavior made results for these cases less accurate (Table I).
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62
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85034876811
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Another possible cause for discrepancy is the adiabatic approximation made in Ref. 47 and Sec. IV:
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68
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0000402997
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edited by H. Ehrenreich, F. Seitz, and D. Turnbull (Academic, New York) For a review see H. Ehrenreich and
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(1976)
Solid State Physics
, vol.31
, pp. 149
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Schwartz, L.M.1
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74
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85034879814
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Note that the rms displacement is normalized to the nearest-neighbor distance rather than a in Ref. 20.
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75
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84950560408
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For [formula omitted] agreement is within 1% or 2%. For smaller λ, particularly [formula omitted] the finite cutoff radius [formula omitted] leads to results which lie as much as 10% below this line. However, this deviation is consistent with lattice dynamics calculations for the effect of [formula omitted] The large λ results extrapolate back to Hansen and Pollock’s result (Ref. 12) at [formula omitted] which was obtained using Ewald sums (i.e., [formula omitted]).
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78
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84950560403
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J. Chem. Phys.
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84
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85034876656
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Effects of counterion correlations and fluctuations on the interaction of charged walls is described by
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89
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85034878334
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Preliminary Monte Carlo studies of the temperature dependent of [formula omitted] for particles interacting with a Yukawa potential are described in
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102
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84950560420
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J. Chem. Phys.
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