scholarly journals Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells

Science ◽  
2006 ◽  
Vol 314 (5806) ◽  
pp. 1757-1761 ◽  
Author(s):  
B. A. Bernevig ◽  
T. L. Hughes ◽  
S.-C. Zhang
2017 ◽  
Vol 19 (7) ◽  
pp. 073031 ◽  
Author(s):  
Zhigang Song ◽  
Sumanta Bose ◽  
Weijun Fan ◽  
Dao Hua Zhang ◽  
Yan Yang Zhang ◽  
...  

2012 ◽  
Vol 85 (12) ◽  
Author(s):  
Paolo Michetti ◽  
Jan C. Budich ◽  
Elena G. Novik ◽  
Patrik Recher

2012 ◽  
Vol 112 (10) ◽  
pp. 103713 ◽  
Author(s):  
M. Baenninger ◽  
M. König ◽  
A. G. F. Garcia ◽  
M. Mühlbauer ◽  
C. Ames ◽  
...  

2014 ◽  
Vol 89 (19) ◽  
Author(s):  
Dong-Hui Xu ◽  
Jin-Hua Gao ◽  
Chao-Xing Liu ◽  
Jin-Hua Sun ◽  
Fu-Chun Zhang ◽  
...  

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Saquib Shamim ◽  
Wouter Beugeling ◽  
Pragya Shekhar ◽  
Kalle Bendias ◽  
Lukas Lunczer ◽  
...  

AbstractSoon after the discovery of the quantum spin Hall effect, it has been predicted that a magnetic impurity in the presence of strong Coulomb interactions will destroy the quantum spin Hall effect. However, the fate of the quantum spin Hall effect in the presence of magnetic impurities has not yet been experimentally investigated. Here, we report the successful experimental demonstration of a quantized spin Hall resistance in HgTe quantum wells dilutely alloyed with magnetic Mn atoms. These quantum wells exhibit an inverted band structure that is very similar to that of the undoped material. Micron sized devices of (Hg,Mn)Te quantum well (in the topological phase) show a quantized spin Hall resistance of h/2e2 at low temperatures and zero magnetic field. At finite temperatures, we observe signatures of the Kondo effect due to interaction between the helical edge channels and magnetic impurities. Our work lays the foundation for future investigations of magnetically doped quantum spin Hall materials towards the realization of chiral Majorana fermions.


2016 ◽  
Vol 49 (5) ◽  
pp. 055305 ◽  
Author(s):  
Ya-ping Wang ◽  
Chang-wen Zhang ◽  
Wei-xiao Ji ◽  
Run-wu Zhang ◽  
Ping Li ◽  
...  

2013 ◽  
Vol 27 (15) ◽  
pp. 1362011 ◽  
Author(s):  
JUN-WON RHIM ◽  
KYUNGSUN MOON

We present here a brief review on the remarkable consequences of the flat bands formed at the edges of the Zigzag graphene nanoribbon (ZGNR). The inclusion of the on-site Coulomb interaction is shown to induce the edge spin ferromagnetism, whose spin stiffness demonstrates a nonmonotonic dependence on the lateral electric field. The critical electric field strength corresponds to that of the insulator to half-metal transition. The inclusion of the spin–orbit coupling (SOC) has been believed to generate the quantum spin Hall effect (QSHE) guiding into the interesting new field of topological insulator. By carefully investigating the SOC near the edge, we have shown that the additional σ-edge band gives a marginal perturbation and hence the existence of the QSHE depends on the coupling strength between the π-edge bands and the σ-edge band. We demonstrate that for the charge neutral ZGNR, the QSHE does not occur in the pristine ZGNR, while the hydrogen passivation along the edge may recover the expected feature of the QSHE.


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