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Volumn 88, Issue 5, 1988, Pages 3286-3312

Phase diagram and dynamics of Yukawa systems

Author keywords

[No Author keywords available]

Indexed keywords


EID: 36549102685     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.453924     Document Type: Article
Times cited : (638)

References (105)
  • 1
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    • For a review of colloidal systems see:
  • 42
    • 85034876093 scopus 로고    scopus 로고
    • 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.
  • 43
    • 85034868288 scopus 로고    scopus 로고
    • While longitudinal phonons of colloidal systems are overdamped by backflow of the fluid, shear modes of small wave vector propagate: see
  • 44
    • 0001383459 scopus 로고
    • 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.
    • (1979) J. Colloid Interface Sci. , vol.71 , pp. 622
    • Joanny, J.F.1
  • 49
    • 85034878700 scopus 로고    scopus 로고
    • See, for example
  • 57
    • 84950560410 scopus 로고    scopus 로고
    • 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).
  • 62
    • 85034876811 scopus 로고    scopus 로고
    • Another possible cause for discrepancy is the adiabatic approximation made in Ref. 47 and Sec. IV:
  • 68
    • 0000402997 scopus 로고
    • edited by H. Ehrenreich, F. Seitz, and D. Turnbull (Academic, New York) For a review see H. Ehrenreich and
    • (1976) Solid State Physics , vol.31 , pp. 149
    • Schwartz, L.M.1
  • 74
    • 85034879814 scopus 로고    scopus 로고
    • Note that the rms displacement is normalized to the nearest-neighbor distance rather than a in Ref. 20.
  • 75
    • 84950560408 scopus 로고    scopus 로고
    • 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]).
  • 78
    • 84950560403 scopus 로고    scopus 로고
    • J. Chem. Phys.
  • 84
    • 85034876656 scopus 로고    scopus 로고
    • Effects of counterion correlations and fluctuations on the interaction of charged walls is described by
  • 89
    • 85034878334 scopus 로고    scopus 로고
    • Preliminary Monte Carlo studies of the temperature dependent of [formula omitted] for particles interacting with a Yukawa potential are described in
  • 102
    • 84950560420 scopus 로고    scopus 로고
    • J. Chem. Phys.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.