Abstract

Geometrically modulated magnetic nanowires are a simple yet efficient strategy to modify the magnetic domain wall propagation since a simple diameter modulation can achieve its pinning during the nanowire magnetization reversal. However, in dense systems of parallel nanowires, the stray fields arising at the diameter interface can interfere with the domain wall propagation in the neighboring nanowires. Therefore, the magnetic behavior of diameter-modulated nanowire arrays can be quite complex and depending on both short and long-range interaction fields, as well as the nanowire geometric dimensions. We applied the first-order reversal curve (FORC) method to bi-segmented Ni nanowire arrays varying the wide segment (45–65 nm diameter, 2.5–10.0 μm length). The FORC results indicate a magnetic behavior modification depending on its length/diameter aspect ratio. The distributions either exhibit a strong extension along the coercivity axis or a main distribution finishing by a fork feature, whereas the extension greatly reduces in amplitude. With the help of micromagnetic simulations, we propose that a low aspect ratio stabilizes pinned domain walls at the diameter modulation during the magnetization reversal. In this case, long-range axial interaction fields nucleate a domain wall at the nanowire extremities, while short-range ones could induce a nucleation at the diameter interface. However, regardless of the wide segment aspect ratio, the magnetization reversal is governed by the local radial stray fields of the modulation near null magnetization. Our findings demonstrate the capacity of distinguishing between complex magnetic behaviors involving convoluted interaction fields.

Highlights

  • Several possible spintronics devices are based on the controlled propagation and manipulation of magnetic domain walls (DWs) along a ferromagnetic nanowire [1]

  • The results showed a major modification of the array magnetization reversal compared to a single-diameter reference array: instead of being governed by a unique mean demagnetizing interaction field, the array magnetic behavior seems to depend upon two competing mean interaction fields

  • The results suggest that, whereas the magnetization reversal effectively occurs through two different interaction fields when the nanowire array is nearly saturated, the diameter modulation stray field of the neighboring nanowires yields a more complex magnetic behavior

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Summary

Introduction

Several possible spintronics devices are based on the controlled propagation and manipulation of magnetic domain walls (DWs) along a ferromagnetic nanowire [1]. The domain wall race-track memory [2,3], where the binary information is recorded as the presence or absence of a magnetic DW, yielded extensive research on the DW behavior [4,5]. Due to their isotropic section, cylindrical magnetic nanowires have been proved to reach faster DW propagation velocities compared with magnetic stripes, without the Walker breakdown phenomenon [6]. Since DW structure arises from an interplay between the exchange and magnetostatic energies, a simple yet efficient way to locally control the DW propagation is through the insertion of geometric discontinuities [7,8,9,10]. 4.0/).

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