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Charge and density fluctuations lock horns: ionic criticality with power-law forces

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Jean-Noël Aqua and Michael E Fisher

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LETTER TO THE EDITOR

How do charge and density fluctuations compete in ionic fluids near gas–liquid criticality when quantum mechanical effects play a role? To gain some insight, long-range \Phi^{\cal L}_{\pm\pm} \big/ r^{d+\sigma} interactions (with σ > 0), which encompass van der Waals forces (when σ = d = 3), have been incorporated in exactly soluble, d-dimensional 1:1 ionic spherical models with charges ±q0 and hard-core repulsions. In accord with previous work, when d > min{σ, 2} (and q0 is not too large), the Coulomb interactions do not alter the (q0 = 0) critical universality class that is characterized by density correlations at criticality decaying as 1/rd−2+η with η = max{0, 2 − σ}. But screening is now algebraic, the charge–charge correlations decaying, in general, only as 1/rd+σ+4; thus σ = 3 faithfully mimics known noncritical d = 3 quantal effects. But in the absence of full (+, −) ion symmetry, density and charge fluctuations mix via a transparent mechanism: then the screening at criticality is weaker by a factor r4−2η. Furthermore, the otherwise valid Stillinger–Lovett sum rule fails at criticality whenever η = 0 (as, e.g., when σ > 2) although it remains valid if η > 0 (as for σ < 2 or in real d ≤ 3 Ising-type systems).


PACS

64.70.F- Liquid–vapor transitions

64.60.Ht Dynamic critical phenomena

02.10.De Algebraic structures and number theory

61.20.Gy Theory and models of liquid structure

82.45.Gj Electrolytes

MSC

15A90 Applications of matrix theory to physics

76M60 Symmetry analysis, Lie group and algebra methods

Subjects

Soft matter, liquids and polymers

Mathematical physics

Condensed matter: structural, mechanical & thermal

Chemical physics and physical chemistry

Dates

Issue 24 (18 June 2004)

Received 6 May 2004

Published 2 June 2004



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