Berit Goodge1,Oscar Gonzalez1,Lilia Xie1,Kwabena Bediako1,2
University of California, Berkeley1,Lawrence Berkeley National Laboratory2
Berit Goodge1,Oscar Gonzalez1,Lilia Xie1,Kwabena Bediako1,2
University of California, Berkeley1,Lawrence Berkeley National Laboratory2
Intercalated transition metal dichalcogenides (TMDs) have been proposed as promising platforms for next-generation spintronic devices based on a wide range of electronic and magnetic phases which can be tuned by varying the host lattice or the species, amount, and ordering of intercalants [1]. Several compounds have been shown to host chiral magnetic order, namely a helical winding of in-plane magnetic moments along the <i>c</i>-axis of the layered crystal structure. Previous studies have shown that different intercalant concentrations can have a dramatic impact on, for example, chiral domains [2] and magnetic properties [3], but a deeper and more predictive understanding of these effects will be necessary for any future applications of these materials. Here, we leverage a combination of imaging modes in the (scanning) transmission electron microscope (S/TEM) to directly probe (dis)order across multiple length scales and show how subtle changes in the atomic lattice can have dramatic impact on mesoscale magnetic textures.<br/><br/><br/>1. Xie, L. S. et al. Structure and Magnetism of Iron- and Chromium-Intercalated Niobium and Tantalum Disulfides. <i>J. Am. Chem. Soc. </i><b>144</b>, 9525−9542 (2022).<br/>2. Horibe, Y. et al. Color Theorems, Chiral Domain Topology, and Magnetic Properties of Fe<i><sub>x</sub></i>TaS<sub>2</sub>. <i>J. Am. Chem. Soc.</i> <b>136</b>, 8368−8373 (2014).<br/>3. Kousaka, Y. et al. An emergence of chiral helimagnetism or ferromagnetism governed by Cr intercalation in a dichalcogenide CrNb<sub>3</sub>S<sub>6</sub>. <i>APL Mater. </i><b>10</b>, 090704 (2022).<br/><br/>* This work supported by University of California President’s Postdoctoral Fellowship Program, the National Science Foundation (DMR-2039380, DMR-1719875, MRI-1429155, DMR-1539918), and the Air Force Office of Scientific Research (FA9550-20-1-0007).