Abstract

The tetragonal compound Mn$_{1.4}$PtSn with the $D_{2d}$ symmetry recently attracted attention as the first known material that hosts magnetic antiskyrmions, which differ from the so far known skyrmions by their internal structure. The latter have been found in a number of magnets with the chiral crystal structure. In previous works, the existence of antiskyrmions in Mn$_{1.4}$PtSn was unambiguously demonstrated in real space by means of Lorentz transmission electron microscopy on thin-plate samples ($\sim$100~nm thick). In the present study, we used small-angle neutron scattering and magnetic force microscopy to perform reciprocal- and real-space imaging of the magnetic texture of bulk Mn$_{1.4}$PtSn single-crystals at different temperatures and in applied magnetic field. We found that the magnetic texture in the bulk differs significantly from that of thin-plate samples. Instead of spin helices or an antiskyrmion lattice, we observe an anisotropic fractal magnetic pattern of closure domains in zero field above the spin-reorientation transition temperature, which transforms into a set of bubble domains in high field. Below the spin-reorientation transition temperature the strong in-plane anisotropy as well as the fractal self-affinity in zero field is gradually lost, while the formation of bubble domains in high field remains robust. The results of our study highlight the importance of dipole-dipole interactions in thin-plate samples for the stabilization of antiskyrmions and identify criteria which should guide the search for potential (anti)skyrmion host materials. Moreover, they provide consistent interpretations of the previously reported magnetotransport anomalies of the bulk crystals.

Highlights

  • Solids exhibiting topological properties are promising for future applications, in particular for spintronics

  • We used a combination of small-angle neutron scattering (SANS) and Magnetic force microscopy (MFM) to study the bulk magnetic structure of Mn1.4PtSn and showed that it differs drastically from what was previously reported from LTEM measurements of thin-plate samples

  • ⇑⇑ ⇑⇓ 3 μm ⇑⇑ ⇑⇓ 3 μm with an anisotropic fractal surface domain pattern that has a characteristic scale with a lower boundary of ∼48 nm and an upper boundary of ∼3 μm defined by the width of the lamellar stripe domains

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Summary

INTRODUCTION

Solids exhibiting topological properties are promising for future applications, in particular for spintronics. Elliptically distorted skyrmions of both handednesses and the nontopological bubble lattice were shown to appear when a symmetry-breaking in-plane magnetic field is applied in combination with the out-of-plane field [29,30] This makes Mn1.4PtSn a unique compound hosting a rich variety of controllable topological magnetic objects. We employ both SANS and MFM to resolve the nanometer-scale magnetic texture of Mn1.4PtSn in the bulk single-crystalline form and observe how it changes when the sample temperature and the applied magnetic field are varied. Instead of helices or an antiskyrmion lattice, we observe an anisotropic fractal magnetic pattern of closure domains in zero field above the spin-reorientation transition temperature TSR, with characteristic hints for the DMI inherent in the D2d symmetry of the crystal, which transforms into a set of bubble domains in high field.

EXPERIMENTAL DETAILS
RESULTS
Domain structure in applied field
DISCUSSION AND CONCLUSIONS
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