AVS 62nd International Symposium & Exhibition
    Magnetic Interfaces and Nanostructures Tuesday Sessions
       Session MI-TuM

Paper MI-TuM12
Abnormal Asymmetric Domain Expansion and Skyrmion Bubble Stability in Thin Films with Strong Dzyaloshinskii-Moriya Interaction

Tuesday, October 20, 2015, 11:40 am, Room 230A

Session: Oxides, Fluorides, and Spin Structures
Presenter: Lucas Caretta, Massachusetts Institute of Technology
Authors: L. Caretta, Massachusetts Institute of Technology
M. Mann, Massachusetts Institute of Technology
AJ. Tan, Massachusetts Institute of Technology
G.S.D. Beach, Massachusetts Institute of Technology
Correspondent: Click to Email

The Dzyaloshinskii-Moriya interaction (DMI) at heavy-metal/ferromagnet interfaces can stabilize chiral spin textures [1]. It has recently been shown that field-driven bubble domain expansion in perpendicularly-magnetized thin films is asymmetric under the application of an in-plane field, which can be used to quantify the DMI effective field in the domain wall (DW) [2]. We have imaged domain expansion in Pt(3nm)/Co(0.9nm)/Pt(x)/GdOx(3nm) films using wide-field Kerr microscopy to characterize this behavior systematically as a function of DMI strength. In the case of null or weak DMI, realized when top and bottom Pt layers are of similar thickness, the in-plane field dependence of the DW velocity is well-described by the simple expansion model derived in Ref. [2]. However, in the case of strong DMI, we find a strongly nonmonotonic behavior due to flattening of the DW, minimizing Zeeman energy and DMI energy. Moreover, we show that when the ratio of the DMI effective field to the perpendicular anisotropy field is large, expanding bubble domains leave behind fine-scale dendritic structures, consisting of coupled 360 degree DWs. These dendritic structures can be manipulated to form stable skyrmion bubbles. We show that the stability of skyrmion bubbles is a strong function of the applied in-plane field near the DMI field. The skyrmion bubble annihilation field becomes deterministic at large in-plane fields.

1. A. Fert et al., Nat. Nano., 8, 152-156 (2013)

2. S.G. Je et al., PRB 88, 214401 (2013)