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To realize the quantum anomalous Hall effect (QAHE) at elevated temperatures, we adopted the approach of magnetic proximity effect (MPE) to break time reversal symmetry in topological insulator (Bi,Sb)2Te3 (BST) based heterostructure with a ferromagnetic insulator like europium iron garnet (EuIG) of perpendicular magnetic anisotropy. Here we demonstrated phenomenally large anomalous Hall resistance (RAHE) as high as 8 {Omega} at 300 K, and sustained to 400 K in 35 BST/EuIG samples, surpassing the past record (0.28 {Omega}) by nearly thirty times. These striking results are attributed to an atomically abrupt interface between BST and EuIG being Fe rich. Importantly, the gate dependence of AHE loop showed no sign change with varying chemical potential, thus the MPE induced AHE is less likely originated from the extrinsic effect. For gate-biased 4 nm BST on EuIG, pronounced topological Hall effect coexisting with AHE were observed at the negative top gate voltage up to 15 K.
The experimental realization of the quantum anomalous Hall (QAH) effect in magnetically-doped (Bi, Sb)2Te3 films stands out as a landmark of modern condensed matter physics. However, ultra-low temperatures down to few tens of mK are needed to reach t
The influence of Sb content, substrate type and cap layers on the quantum anomalous Hall effect observed in V-doped (Bi,Sb)$_2$Te$_3$ magnetic topological insulators is investigated. Thin layers showing excellent quantization are reproducibly deposit
The amorphous iron-germanium system ($a$-Fe$_x$Ge$_{1-x}$) lacks long-range structural order and hence lacks a meaningful Brillouin zone. The magnetization of aFeGe is well explained by the Stoner model for Fe concentrations $x$ above the onset of ma
The Berry phase picture provides important insights into the electronic properties of condensed matter systems. The intrinsic anomalous Hall (AH) effect can be understood as a consequence of non-zero Berry curvature in momentum space. The realization
Quantum anomalous Hall effect(QAHE) can only be realized at extremely low temperatures in magnetically doped topological insulators(TIs) due to limitations inherent with the doping precess. In an effort to boost the quantization temperature of QAHE,