Jean-Noël Aqua and Michael E Fisher 2004 J. Phys. A: Math. Gen. 37 L241 doi:10.1088/0305-4470/37/24/L02
Jean-Noël Aqua and Michael E Fisher
Show affiliationsHow 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
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).
64.70.F- Liquid–vapor transitions
64.60.Ht Dynamic critical phenomena
02.10.De Algebraic structures and number theory
Soft matter, liquids and polymers
Issue 24 (18 June 2004)
Received 6 May 2004
Published 2 June 2004
Jean-Noël Aqua and Michael E Fisher 2004 J. Phys. A: Math. Gen. 37 L241
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