Abstract

While the magnetic properties of nanoscaled antidot lattices in in-plane magnetized materials have widely been investigated, much less is known about the microscopic effect of hexagonal antidot lattice patterning on materials with perpendicular magnetic anisotropy. By using a combination of first-order reversal curve measurements, magnetic x-ray microscopy, and micromagnetic simulations we elucidate the microscopic origins of the switching field distributions that arise from the introduction of antidot lattices into out-of-plane magnetized GdFe thin films. Depending on the geometric parameters of the antidot lattice we find two regimes with different magnetization reversal processes. For small antidots, the reversal process is dominated by the exchange interaction and domain wall pinning at the antidots drives up the coercivity of the system. On the other hand, for large antidots the dipolar interaction is dominating which leads to fragmentation of the system into very small domains that can be envisaged as a basis for a bit patterned media.

Highlights

  • Periodic arrangements of holes, so called antidot lattices, in thin magnetic films have been broadly investigated in various host materials

  • JOACHIM GRA FE et al Here, we describe the influence of nanoscaled antidot structuring with different geometries on the magnetic properties of soft-magnetic GdFe thin films with perpendicular magnetic anisotropy

  • We discuss these properties of the two antidot lattice geometries using a combination of first-order reversal curve (FORC) measurements, scanning x-ray microscopy (SXM) imaging and micromagnetic simulations to gain a complete microscopic understanding

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Summary

Introduction

Called antidot lattices, in thin magnetic films have been broadly investigated in various host materials. Antidot lattices are investigated in magnetic thin films with in-plane anisotropy where the strong influence of the nanostructures due to emergent demagnetization fields at the hole edges is obvious [12]. This is widely used to tune the magnetic anisotropy [13,14,15] and coercivity [16,17,18] of these thin films, and the microscopic origin is well established in literature [15,19,20,21,22,23,24]. To gain an understanding of the processes involved in the magnetization reversal a multitude of approaches have been combined, namely, micromagnetic simulations [15,19,20], magneto-optical Kerr effect (MOKE)

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