TY - JOUR
T1 - Renormalization group calculations for wetting transitions of infinite order and continuously varying order
T2 - Local interface Hamiltonian approach
AU - Indekeu, J. O.
AU - Koga, K.
AU - Hooyberghs, H.
AU - Parry, A. O.
N1 - Copyright:
Copyright 2013 Elsevier B.V., All rights reserved.
PY - 2013/8/13
Y1 - 2013/8/13
N2 - We study the effect of thermal fluctuations on the wetting phase transitions of infinite order and of continuously varying order, recently discovered within a mean-field density-functional model for three-phase equilibria in systems with short-range forces and a two-component order parameter. Using linear functional renormalization group calculations within a local interface Hamiltonian approach, we show that the infinite-order transitions are robust. The exponential singularity (implying 2-αs=∞) of the surface free energy excess at infinite-order wetting as well as the precise algebraic divergence (with βs=-1) of the wetting layer thickness are not modified as long as ω<2, with ω the dimensionless wetting parameter that measures the strength of thermal fluctuations. The interface width diverges algebraically and universally (with ν⊥=1/2). In contrast, the nonuniversal critical wetting transitions of finite but continuously varying order are modified when thermal fluctuations are taken into account, in line with predictions from earlier calculations on similar models displaying weak, intermediate, and strong fluctuation regimes.
AB - We study the effect of thermal fluctuations on the wetting phase transitions of infinite order and of continuously varying order, recently discovered within a mean-field density-functional model for three-phase equilibria in systems with short-range forces and a two-component order parameter. Using linear functional renormalization group calculations within a local interface Hamiltonian approach, we show that the infinite-order transitions are robust. The exponential singularity (implying 2-αs=∞) of the surface free energy excess at infinite-order wetting as well as the precise algebraic divergence (with βs=-1) of the wetting layer thickness are not modified as long as ω<2, with ω the dimensionless wetting parameter that measures the strength of thermal fluctuations. The interface width diverges algebraically and universally (with ν⊥=1/2). In contrast, the nonuniversal critical wetting transitions of finite but continuously varying order are modified when thermal fluctuations are taken into account, in line with predictions from earlier calculations on similar models displaying weak, intermediate, and strong fluctuation regimes.
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U2 - 10.1103/PhysRevE.88.022122
DO - 10.1103/PhysRevE.88.022122
M3 - Article
AN - SCOPUS:84883876741
VL - 88
JO - Physical Review E
JF - Physical Review E
SN - 2470-0045
IS - 2
M1 - 022122
ER -