Finite-size Kosterlitz-Thouless transition in 2DXY Fe/W(001) ultrathin films
arXiv:1811.09238 · doi:10.1103/PhysRevB.99.125425
Abstract
Magnetic susceptibility measurements of 3-4 ML Fe/W(001) ferromagnetic films demonstrate that this is a 2DXY system in which a finite-size Kosterlitz-Thouless (KT) transition occurs. The films are grown in ultrahigh vacuum and their magnetic response is measured using the magneto-optic Kerr effect (MOKE). The analysis of many independently grown films shows that the paramagnetic tail of the susceptibility is described by $χ(T) \sim \exp \bigr{(}B/(T/T_{KT}-1)^a\bigl{)}$, where and , in quantitative agreement with KT theory. Below the finite-size transition temperature , the behavior is complicated by dissipation (likely related to the re-emergence of fourfold anisotropy and magnetic domains). A subset of measurements with very small dissipation most closely represents the idealized system treated by theory. In these, the temperature interval between the fitted Kosterlitz-Thouless transition temperature and the finite-size transition temperature is . This yeids an estimate of the finite size affecting the film of order micrometers. This gives experimental support to the idea that even a mesoscopic limitation of the vortex-antivortex gas results in a substantial finite-size effect at the KT transition. In contrast, fitting the paramagnetic tail to a power law, appropriate to a second order critical transition, does not give reasonable results. The effective critical exponent does not correspond to a known universality class, and the fitted transition temperature is much further below the peak in the susceptibility than is reasonable.
arXiv comment9 pages, 4 figures
References in corpus (4)
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Cited by in corpus (3)
- Intrinsic 2D-XY ferromagnetism in a van der Waals monolayer
- Renormalization group analysis of the finite 2DXY model with fourfold anisotropy: Application to the magnetic susceptibility of a ferromagnetic ultrathin film
- Classical fully-packed loop model with attractive interactions on the square lattice