Critical Casimir amplitudes for -component models with O(n)-symmetry breaking quadratic boundary terms
arXiv:0905.3113 · doi:10.1016/j.nuclphysb.2009.07.010
Abstract
Euclidean -component theories whose Hamiltonians are O(n) symmetric except for quadratic symmetry breaking boundary terms are studied in films of thickness . The boundary terms imply the Robin boundary conditions at the boundary planes at and . Particular attention is paid to the cases in which of the variables take the special value corresponding to critical enhancement while the remaining ones are subcritically enhanced. Under these conditions, the semi-infinite system bounded by has a multicritical point, called -special, at which an symmetric critical surface phase coexists with the O(n) symmetric bulk phase, provided is sufficiently large. The -dependent part of the reduced free energy per area behaves as as at the bulk critical point. The Casimir amplitudes are determined for small in the general case where components are critically enhanced at both boundary planes, components are enhanced at one plane but satisfy asymptotic Dirichlet boundary conditions at the respective other, and the remaining components satisfy asymptotic Dirichlet boundary conditions at both . Whenever , these expansions involve integer and fractional powers with (mod logarithms). Results to for general values of , , and are used to estimate the of 3D Heisenberg systems with surface spin anisotropies when , , and .
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