Equilibrium spin-glass transition of magnetic dipoles with random anisotropy axes

dc.creatorFernández, J. F.
dc.date2009-03-04
dc.date.accessioned2026-07-07T12:49:00Z
dc.date.available2026-07-07T12:49:00Z
dc.descriptionWe study fully occupied lattice systems of classical magnetic dipoles which point along random axes. Only dipolar interactions are considered. From tempered Monte Carlo simulations, we obtain numerical evidence that supports the following conclusions: in three dimensions, (a) there is an equilibrium spin glass phase at temperatures below $T_c$, where $k_BT_c= (0.86\pm 0.07)\varepsilon_d $ and $\varepsilon_d$ is a nearest neighbor dipole-dipole interaction energy, (b) in the spin glass phase the overlap parameter is approximately given by $\sqrt{1-T/T_c}$, and (c) the correlation length $ξ$ diverges at $T_c$ with a critical exponent $ν=1.5\pm0.5$; in two dimensions $ξ$ diverges at or near T=0 and $ν=3\pm1$.
dc.description6 pages, 8 figures
dc.identifierhttps://arxiv.org/abs/0903.0709
dc.identifierhttp://arxiv.org/abs/0903.0709
dc.identifierPhys. Rev. B 78, 064404 (2008)
dc.identifierdoi:10.1103/PhysRevB.78.064404
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/222254
dc.subjectMaterials Science
dc.subjectDisordered Systems and Neural Networks
dc.titleEquilibrium spin-glass transition of magnetic dipoles with random anisotropy axes
dc.typetext

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