Abstract

Hexagonal antidot arrays have been patterned on weak perpendicular magnetic anisotropy NdCo films by e-beam lithography and lift off. Domain structure has been characterized by Magnetic Force Microscopy at remanence. On a local length scale, of the order of stripe pattern period, domain configuration is controlled by edge effects within the stripe pattern: stripe domains meet the hole boundary at either perpendicular or parallel orientation. On a longer length scale, in-plane magnetostatic effects dominate the system: clear superdomains are observed in the patterned film with average in-plane magnetization along the easy directions of the antidot array, correlated over several antidot array cells.

Highlights

  • Magnetic antidots have often been used to tailor the magnetic properties of extended films:[1,2,3,4,5,6,7,8,9,10,11,12] Depending on hole size and array geometry, they can enhance DW pinning,[2] modify magnetic anisotropy and easy axis direction[3] or, even, create ratchet effects on DW propagation.[4]

  • We have studied the effects of the magnetostatic shape anisotropy of a patterned antidot array on the remanent stripe domain configuration of perforated Weak perpendicular magnetic anisotropy (wPMA) NdCo films with hole size comparable to stripe domain periods

  • This indicates the uniform orientation of the average in-plane magnetization in the observed region (Fig. 2(a)). This configuration minimizes “rotatable anisotropy”, that in wPMA materials tends to align the stripes with the last saturating field direction.[15]. It is favored by magnetostatic shape anisotropy of the antidot array, since this array direction was found to be an easy axis for in-plane magnetized hexagonal arrays of permalloy antidots.[3]

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Summary

INTRODUCTION

Magnetic antidots have often been used to tailor the magnetic properties of extended films:[1,2,3,4,5,6,7,8,9,10,11,12] Depending on hole size and array geometry, they can enhance DW pinning,[2] modify magnetic anisotropy and easy axis direction[3] or, even, create ratchet effects on DW propagation.[4] For magnetic materials with in-plane anisotropy (i.e. magnetization confined to sample plane), magnetostatic effects at hole boundaries create periodic closure domain structures[1,3,5] with enhanced stability by the presence of pairs of half-vortices confined to hole edges.[6] magnetization reversal occurs by the propagation of “composite DWs” that separate regions with different orientations of the closure domain structure relative to the applied field directions, so called “superdomains”.7,8. On a longer length scale, “superdomains” are clearly observed, with average in-plane magnetization along the easy axis directions for in-plane shape anisotropy

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