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Magnetic dipolar interaction in ultrathin films: Structural and size effects
- Source :
- Journal of Magnetism and Magnetic Materials. 321:2150-2159
- Publication Year :
- 2009
- Publisher :
- Elsevier BV, 2009.
-
Abstract
- A previously introduced formalism for calculating magnetic dipolar anisotropy energy Δ U in atomic layered structures is further developed. Numerical results are presented for ultrathin films with different close-packed (face centered cubic (FCC) [1 1 1]) and non-close-packed (FCC [0 0 1] and body centered cubic (BCC) [0 0 1]) structures. Structural effects become apparent in the magnetocrystalline dipolar anisotropy energy Δ U L when the ratio between the interlayer separation c and the 2D lattice constant a is changed. Despite the long-range character of the dipolar interaction, it is shown that the number of significantly interacting layers, conventially called coupled layers, is limited and depends on the structural aspect ratio c / a . The slope in the observed linear dependence between Δ U L and the inverse of the film thickness t is explained by the number of the so-called coupled layers, and not by a surface contribution to volume values. Size effects appearing in Δ U are unambiguously distinguished from structural effects. Effective anisotropy energy Δ U eff and Δ U are presented for Co [0 0 0 1] and Ni [0 0 1] ultrathin films. It is verified that the dipolar interaction makes an important contribution to Δ U eff , but the spin reorientation transition is determined by non-dipolar interactions. The former favors the magnetization switching only when the size aspect ratio d / t , with d the characteristic lateral dimension of the film, is sufficiently small. Applications to other layered arrays of magnetic dipoles are straightforward.
Details
- ISSN :
- 03048853
- Volume :
- 321
- Database :
- OpenAIRE
- Journal :
- Journal of Magnetism and Magnetic Materials
- Accession number :
- edsair.doi...........0c97ea01f2d7e38a2f6646dd5eb3b8e9
- Full Text :
- https://doi.org/10.1016/j.jmmm.2009.01.009