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Physical Review Letters

Volumn 65, Issue 27, 1990, Pages 3405-3408

Fluid interface tensions near critical end points

(2) Fisher, Michael E a Upton, Paul J a

a UNIVERSITY OF MARYLAND (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 5544227735 PISSN: 00319007 EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevLett.65.3405 Document Type: Article

Times cited : (84)

References (27)

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- One must distinguish symmetric and nonsymmetric end points (Ref. 1): Only the latter are considered here.

5
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- See J. S. Rowlinson and B. Widom, Molecular Theory of Capillarity (Oxford Univ. Press, London, 1982), Secs. 8.3, 9.6, etc.;

6
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- Noncritical interface near a critical end point II
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10
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- We also use δ = 1 + γ / beta, 2 - η = γ / nu, and dstar= ( 2 - α ) / nu (= d for d <= 4). The context should obviate confusion between exponents alpha, beta, and gamma and the phases so labeled.

11
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12
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- Phys. Rev. B (to be published)study spherical models but these have no proper interfaces.
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13
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- Structure and Free Energy of the Interface between Fluid Phases in Equilibrium near the Critical Point
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14
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- Here theta is the leading correction-to-scaling exponent.

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16
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- We let k0, k1, ~.~.~ denote distinct constants.

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27
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- G. W. Mulholland [Ph.D. thesis, Cornell University, 1973 (unpublished)] has made related studies, unsuccessful mainly, we feel, because such a reduction was not required.

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