2020
DOI: 10.1002/adma.202001460
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Observation of Quantum Anomalous Hall Effect and Exchange Interaction in Topological Insulator/Antiferromagnet Heterostructure

Abstract: Integration of a quantum anomalous Hall insulator with a magnetically ordered material provides an additional degree of freedom through which the resulting exotic quantum states can be controlled. Here, an experimental observation is reported of the quantum anomalous Hall effect in a magnetically‐doped topological insulator grown on the antiferromagnetic insulator Cr2O3. The exchange coupling between the two materials is investigated using field‐cooling‐dependent magnetometry and polarized neutron reflectometr… Show more

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Cited by 36 publications
(42 citation statements)
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References 28 publications
(31 reference statements)
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“…erg. While the magnitude of the exchange bias eld observed here is comparable to what has been previously reported in the Cr 2 O 3 /CBST system, [31] the size of J eb is three orders of magnitude smaller than typical perpendicularly exchange-biased FM/AFM systems such as [Pt/Co]/Cr 2 O 3 and [Pt/Co]/IrMn, where the exchange couplings are believed to be short-range interactions. [32,33] In summary, we have studied the magnetization dynamics of Cr 0.26 (Bi 0.3 Sb 0.7 ) 1.74 Te 3 /CrSb bilayer system using ultrafast magneto-optical techniques.…”
Section: Discussionsupporting
confidence: 80%
“…erg. While the magnitude of the exchange bias eld observed here is comparable to what has been previously reported in the Cr 2 O 3 /CBST system, [31] the size of J eb is three orders of magnitude smaller than typical perpendicularly exchange-biased FM/AFM systems such as [Pt/Co]/Cr 2 O 3 and [Pt/Co]/IrMn, where the exchange couplings are believed to be short-range interactions. [32,33] In summary, we have studied the magnetization dynamics of Cr 0.26 (Bi 0.3 Sb 0.7 ) 1.74 Te 3 /CrSb bilayer system using ultrafast magneto-optical techniques.…”
Section: Discussionsupporting
confidence: 80%
“…[ 204 ] However, the heterostructure effectively engineers a long‐range exchange coupling between the MTI layers using the AFM layer with Néel temperature up to ≈700 K. Heterostructure of AFM and MTI may also lead to additional manipulation of the quantum anomalous Hall insulator (QAHI) state through exchange bias effect. [ 205 ]…”
Section: Recent Results In Topological Insulator (Ti) – Magnetic Materials (Mm) Heterostructuresmentioning
confidence: 99%
“…Recently, by further optimizing the interfacial magnetic proximity effect, the quantum anomalous Hall effect with tunable Chern numbers has also been realized in the emergent MTI heterostructures [65][66][67]]. Following the concept of magnetic insulator with non-zero Chern number elaborated in Section 1, a novel FMI/TI/FMI sandwich heterostructure of (Zn,Cr)Te/(Bi,Sb) 2 Te 3 /(Zn,Cr)Te is grown by MBE, as illustrated in Figure 8a [66].…”
Section: Towards High-t C Topological Insulators-based Magnetic Heterostructuresmentioning
confidence: 99%
“…The resulting strong magnetic exchange interaction at both TI/FMI interface thereafter opens the exchange gap of the TI surface states, and gives rise to the dissipationless chiral edge conduction when all dissipative channels in the (Zn,Cr)Te and (Bi,Sb) 2 Te 3 bulk layers are suppressed at 30 mK (Figure 8b). Additionally, the preparation of single-crystalline Cr 2 O 3 thin film with perpendicular spin-polarized surface by MBE can also introduce highly efficient interfacial exchange coupling in the Cr-doped (Bi x Sb 1−x ) 2 Te 3 /Cr 2 O 3 bilayer sample (Figure 8c) [65]. Consequently, the induced exchange bias effect provides another degree of freedom to manipulate the QAH states in the TI-based magnetic heterostructures.…”
Section: Towards High-t C Topological Insulators-based Magnetic Heterostructuresmentioning
confidence: 99%