Unexpected edge conduction in mercury telluride quantum wells under broken time-reversal symmetry

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作者
Eric Yue Ma
M. Reyes Calvo
Jing Wang
Biao Lian
Mathias Mühlbauer
Christoph Brüne
Yong-Tao Cui
Keji Lai
Worasom Kundhikanjana
Yongliang Yang
Matthias Baenninger
Markus König
Christopher Ames
Hartmut Buhmann
Philipp Leubner
Laurens W. Molenkamp
Shou-Cheng Zhang
David Goldhaber-Gordon
Michael A. Kelly
Zhi-Xun Shen
机构
[1] Geballe Laboratory for Advanced Materials,Department of Applied Physics
[2] Stanford University,Department of Physics
[3] 476 Lomita Mall,Department of Physics
[4] Stanford,undefined
[5] California 94305,undefined
[6] USA,undefined
[7] Stanford University,undefined
[8] 348 Via Pueblo Mall,undefined
[9] Stanford,undefined
[10] California 94305,undefined
[11] USA,undefined
[12] Stanford University,undefined
[13] 382 Via Pueblo Mall,undefined
[14] Stanford,undefined
[15] California 94305,undefined
[16] USA,undefined
[17] Physikalisches Institut (EP3),undefined
[18] Universität Würzburg,undefined
[19] University of Texas at Austin,undefined
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摘要
The realization of quantum spin Hall effect in HgTe quantum wells is considered a milestone in the discovery of topological insulators. Quantum spin Hall states are predicted to allow current flow at the edges of an insulating bulk, as demonstrated in various experiments. A key prediction yet to be experimentally verified is the breakdown of the edge conduction under broken time-reversal symmetry. Here we first establish a systematic framework for the magnetic field dependence of electrostatically gated quantum spin Hall devices. We then study edge conduction of an inverted quantum well device under broken time-reversal symmetry using microwave impedance microscopy, and compare our findings to a non-inverted device. At zero magnetic field, only the inverted device shows clear edge conduction in its local conductivity profile, consistent with theory. Surprisingly, the edge conduction persists up to 9 T with little change. This indicates physics beyond simple quantum spin Hall model, including material-specific properties and possibly many-body effects.
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