We show that edge-state transport in semiconductor-based quantum spin Hall systems is unexpectedly robust to magnetic fields. The origin for this robustness lies in an intrinsic suppression of the edge-state g-factor and the fact that the edge-state Dirac point is typically hidden in the valence band. A detailed k.p band-structure analysis reveals that both InAs/GaSb and HgTe/CdTe quantum wells exhibit such buried Dirac points for a wide range of well thicknesses. By simulating transport in a disordered system described within an effective model, we demonstrate that edge-state transport remains nearly quantized up to large magnetic fields, consistent with recent experiments.
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Department of Applied Physics, Stanford University, Stanford
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo ParkDepartment of Applied Physics, Stanford University, Stanford
Nowack K.C.
Spanton E.M.
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Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park
Department of Physics, Stanford University, StanfordDepartment of Applied Physics, Stanford University, Stanford
Spanton E.M.
Baenninger M.
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Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park
Department of Physics, Stanford University, StanfordDepartment of Applied Physics, Stanford University, Stanford
Baenninger M.
König M.
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Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park
Department of Physics, Stanford University, StanfordDepartment of Applied Physics, Stanford University, Stanford
König M.
Kirtley J.R.
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Department of Applied Physics, Stanford University, StanfordDepartment of Applied Physics, Stanford University, Stanford
Kirtley J.R.
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Kalisky B.
Ames C.
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Physikalisches Institut (EP3), Universität Würzburg, Am Hubland, D-97074, WürzburgDepartment of Applied Physics, Stanford University, Stanford
Ames C.
Leubner P.
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Physikalisches Institut (EP3), Universität Würzburg, Am Hubland, D-97074, WürzburgDepartment of Applied Physics, Stanford University, Stanford
Leubner P.
Brüne C.
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Physikalisches Institut (EP3), Universität Würzburg, Am Hubland, D-97074, WürzburgDepartment of Applied Physics, Stanford University, Stanford
Brüne C.
Buhmann H.
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Physikalisches Institut (EP3), Universität Würzburg, Am Hubland, D-97074, WürzburgDepartment of Applied Physics, Stanford University, Stanford
Buhmann H.
Molenkamp L.W.
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Physikalisches Institut (EP3), Universität Würzburg, Am Hubland, D-97074, WürzburgDepartment of Applied Physics, Stanford University, Stanford
Molenkamp L.W.
Goldhaber-Gordon D.
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Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park
Department of Physics, Stanford University, StanfordDepartment of Applied Physics, Stanford University, Stanford
Goldhaber-Gordon D.
Moler K.A.
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Department of Applied Physics, Stanford University, Stanford
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park
Department of Physics, Stanford University, StanfordDepartment of Applied Physics, Stanford University, Stanford