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. 2020 Jul 22;6(30):eaba4275. doi: 10.1126/sciadv.aba4275

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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. 2 — As a comparison, physical properties of MnBi₆Te₁₀ are also shown. (A and B) Temperature-dependent susceptibility taken at H = 0.1 kOe for MnBi₈Te₁₃ (A) and MnBi₆Te₁₀ (B). Inset: Temperature-dependent specific heat: (A) MnBi₈Te₁₃ and (B) MnBi₆Te₁₀. The criterion to determine T_c and T_N is shown in the inset. (C and D) Magnetic hysteresis loop of isothermal magnetization at low fields with H ⊥ c for MnBi₈Te₁₃ (C) and MnBi₆Te₁₀ (D). (E and F) Magnetic hysteresis loop of isothermal magnetization up to 7 T with H ⊥ c and H ⊥ ab: MnBi₈Te₁₃ (E) and MnBi₆Te₁₀ (F). (G and H) Anisotropic resistivity, ρ_xx and ρ_zz, for MnBi₈Te₁₃ (G) and MnBi₆Te₁₀ (H).