2016
DOI: 10.1103/physrevb.93.155160
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Emergence of magnetic topological states in topological insulators doped with magnetic impurities

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Cited by 11 publications
(20 citation statements)
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“…Since the discovery of TIs, considerable experimental effort has been dedicated to achieve long-range magnetic order in two prototypical TIs, Bi 2 Se 3 and Bi 2 Te 3 , by doping with different TM atoms, such as Cr, Mn, or Fe, in both bulk and thin film geometries [17][18][19][20][21][22][23][24][25][26][27]. Significant theoretical work has also been undertaken to understand the mechanism of magnetism in transition metal (TM) doped TIs [28][29][30][31][32][33][34][35][36][37][38][39][40][41][42][43]. For some of the magnetic TIs where the QAHE has been observed, such as Cr-doped (Bi,Sb) 2 Te 3 , it has been proposed that the mechanism driving the ferromagnetic transition is based on the Van Vleck spin susceptibility [4].…”
Section: Introductionmentioning
confidence: 99%
“…Since the discovery of TIs, considerable experimental effort has been dedicated to achieve long-range magnetic order in two prototypical TIs, Bi 2 Se 3 and Bi 2 Te 3 , by doping with different TM atoms, such as Cr, Mn, or Fe, in both bulk and thin film geometries [17][18][19][20][21][22][23][24][25][26][27]. Significant theoretical work has also been undertaken to understand the mechanism of magnetism in transition metal (TM) doped TIs [28][29][30][31][32][33][34][35][36][37][38][39][40][41][42][43]. For some of the magnetic TIs where the QAHE has been observed, such as Cr-doped (Bi,Sb) 2 Te 3 , it has been proposed that the mechanism driving the ferromagnetic transition is based on the Van Vleck spin susceptibility [4].…”
Section: Introductionmentioning
confidence: 99%
“…The details of numerical calculations are presented elsewhere [10]. Actually, we treat the localized electron spin classically and set S 2 i = 1 as usually adopted in many studies of magnetic materials [20][21][22][23][24][25][26][27][28][29][30][31][32][33]. We calculate Ω for different trial states which are generated by all arranges of localized electron spins within the 3 × 3 unit cell, and find its lowest value [10].…”
Section: Bogoliubov Variational Principle and Numerical Resultsmentioning
confidence: 99%
“…The Hund coupling essentially describes the double exchange processes between itinerant electrons and localized spins [14,15]. As widely adopted in the studies of magnetic materials, we will treat the localized spins classically [14,15,[21][22][23][24][25][26][27][28][29][30][31][32].In addition, we omit the nearest-neighbor interactions between itinerant electrons and localized spins. They would be weaker than the local Hund coupling.…”
Section: Modelmentioning
confidence: 99%
“…It (Φ ≠ 0, π) induces topologically nontrivial band structure [4,5]. When the Hund coupling is included, its interplay with the SOC can emerge topological magnetic phases [31,32]. Hamiltonian (2) is just the spin version of the quantum anomalous Hall model, which is obtained from the double exchange model in the strong Hund coupling limit [4].…”
Section: Modelmentioning
confidence: 99%