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. 2020 Jul 24;6(30):eabb9379. doi: 10.1126/sciadv.abb9379

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Copyright © 2020 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

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Fig. 6 — (A) Magnetization plotted as a function of field in CrCl_0.8Br_1.2I_1.0. The red and blue data correspond to the field perpendicular (B_⊥) and parallel (B_∥) to the honeycomb layers, respectively. The saturated moment is consistent with S = 3/2 in Cr³⁺. (B) Magnified view of the spin-canting transition at B_⊥ = 0.7 T. (C) Optical image, scanning electron microscope (SEM) image, and energy-dispersive x-ray spectroscopy (EDX) color maps reveal a uniform distribution of Cr (yellow, K-edge), Cl (green, K-edge), Br (red, L-edge), and I (blue, L-edge) in CrCl_0.8Br_1.2I_1.0. Photo credit: F.T., Boston College.