Abstract

Vortex domain walls poses chirality or ‘handedness’ which can be exploited to act as memory units by changing their polarity with electric field or driving/manupulating the vortex itself by electric currents in multiferroics. Recently, domain walls formed by one dimensional array of vortex—like structures have been theoretically predicted to exist in disordered rare-earth helical magnets with topological defects. Here, in this report, we have used a combination of two rare-earth metals, e.g. superlattice that leads to long range magnetic order despite their competing anisotropies along the out-of-plane (Er) and in-plane (Tb) directions. Probing the vertically correlated magnetic structures by off-specular polarized neutron scattering we confirm the existence of such magnetic vortex—like domains associated with magnetic helical ordering within the Er layers. The vortex—like structures are predicted to have opposite chirality, side—by—side, and are fairly unaffected by the introduction of magnetic ordering between the interfacial Tb layers and also with the increase in magnetic field which is a direct consequence of screening of the vorticity in the system due to a helical background. Overall, the stability of these vortices over a wide range of temperatures, fields and interfacial coupling, opens up the opportunity for fundamental chiral spintronics in unconventional systems.

Highlights

  • 229–221 K, below which it orders ferromagnetically with an easy axis along the a-axis

  • Off-specular scattering contributions along the in-plane momentum transfer vector q cos(αi)] arise, when the in-plane translational symmetry is broken by interface waviness or by magnetic domains on a length scale shorter than the in-plane projection of the neutron coherence length l along q (=qx, qy )[16,17]

  • In the present experimental geometry, only qx is resolved whereas signal along qy is integrated

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Summary

Methods

The neutron scattering experiments were performed at the polarized neutron reflectometer with polarization analysis HADAS at the Jülich research reactor FRJ-2 (DIDO). The details of the instrument and scattering geometry has been described in Ref. 19, 20. Multilayers with the full layer sequence [Er21 /Tb5 ]. The indices denote the number of atomic layers. The sample was grown with the hexagonal(0001) direction parallel to the surface normal, i.e. parallel to the propagation vector of magnetization. Details of the sample growth and characterization have been published earlier[14]. For the magnetization measurement a small piece has been cut from the sample used for the neutron scattering experiments. A SQUID magnetometer (MPMS set-up from Quantum Design) has been used to study the temperature dependent magnetization for different applied fields

Results
Discussion
Conclusion

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