Fluctuation-induced forces in strongly anisotropic critical systems

Details Fluctuation-induced forces in strongly anisotropic critical systems Fluctuation-induced forces in strongly anisotropic critical systems

2010-08-25

arxiv.org/abs/1008.4241v3

J.Stat.Mech.1011:P11020,2010

Physics

Condensed Matter

Statistical Mechanics

LaTeX source file with 10 eps files, thereof 2 figures, 41 pages; corrected misprints and incorporated ERRATUM

Scientific paper

10.1088/1742-5468/2010/11/P11020

Strongly anisotropic critical systems are considered in a $d$-dimensional film geometry. Such systems involve two (or more) distinct correlation lengths $\xi_\beta$ and $\xi_\alpha$ that scale as nontrivial powers of each other, i.e.\ $\xi_\alpha\sim\xi_\beta^\theta$ with anisotropy index $\theta\ne 1$. Thus two fundamental orientations, perpendicular ($\perp$) and parallel ($\|$), for which the surface normal is oriented along an $\alpha$- and $\beta$-direction, respectively, must be distinguished. The confinement of critical fluctuations caused by the film's boundary planes is shown to induce effective forces $\mathcal{F}_C$ that decay as $\mathcal{F}_C\propto-(\partial/\partial L)\Delta_{\perp,\|}\,L^{-\zeta_{\perp,\|}}$ as the film thickness $L$ becomes large, where the proportionality constants involve nonuniversal amplitudes. The decay exponents $\zeta_{\perp,\|}$ and the Casimir amplitudes $\Delta_{\perp,\|}$ are universal but depend on the type of orientation. To corroborate these findings, $n$-vector models with an $m$-axial bulk Lifshitz point are investigated by means of RG methods below the upper critical dimension $d^*(m)=4+m/2$ under various boundary conditions (BC). The exponents $\zeta_{\perp,\|}$ are determined, and explicit results to one- or two-loop order are presented for several Casimir amplitudes $\Delta^{\mathrm{BC}}_{\perp,\|}$. The large-$n$ limits of the Casimir amplitudes $\Delta_{\|}^{\mathrm{BC}}/n$ for periodic and Dirichlet BC are shown to be proportional to their critical-point analogues at dimension $d-m/2$. The limiting values $\Delta^{\mathrm{PBC}}_{\|,\perp,\infty}=\lim_{n\to\infty}\Delta_{\|,\perp}^{\mathrm{PBC}}/n$ are determined exactly for the uniaxial cases $(d,m)=(3,1)$ under periodic BC. Unlike $\Delta^{\mathrm{PBC}}_{\|,\infty}$, $\Delta^{\mathrm{PBC}}_{\perp,\infty}$ is positive, so that the corresponding Casimir force is repulsive.

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