2014
DOI: 10.1103/physrevb.89.201403
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Synthetic helical liquid in a quantum wire

Abstract: We show that the combination of a Dresselhaus interaction and a spatially periodic Rashba interaction leads to the formation of a helical liquid in a quantum wire when the electron-electron interaction is weakly screened. The effect is sustained by a helicity-dependent effective band gap which depends on the size of the Dresselhaus and Rashba spin-orbit couplings. We propose a design for a semiconductor device in which the helical liquid can be realized and probed experimentally

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Cited by 10 publications
(10 citation statements)
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“…The HLL put forward in Ref. 43 is different from the ones that have so far been studied experimentally: It is neither holographic 40 (unlike the edge states of a quantum spin Hall insulator) nor quasihelical 55 (unlike a magnetic-field-assisted helical liquid). The timereversal analog of the fermion-doubling problem implied by Kramers' theorem 40 is instead avoided by the fact that the gapped branch breaks time-reversal symmetry spontaneously by developing a spin-density wave (SDW).…”
Section: B Bosonized Theorymentioning
confidence: 93%
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“…The HLL put forward in Ref. 43 is different from the ones that have so far been studied experimentally: It is neither holographic 40 (unlike the edge states of a quantum spin Hall insulator) nor quasihelical 55 (unlike a magnetic-field-assisted helical liquid). The timereversal analog of the fermion-doubling problem implied by Kramers' theorem 40 is instead avoided by the fact that the gapped branch breaks time-reversal symmetry spontaneously by developing a spin-density wave (SDW).…”
Section: B Bosonized Theorymentioning
confidence: 93%
“…In Ref. 43 we analyzed the bosonized theory defined by Eqs. ( 18)-( 20) in the absence of superconducting pairing, i.e.…”
Section: B Bosonized Theorymentioning
confidence: 99%
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“…[31][32][33][34][35] for various semiconductor based approximate realizations), there is a priori no topological protection against elastic single particle back-scattering by TRS and the extent to which the correlation functions concur with Eqs. (1-2) has not been checked from first principles yet.…”
Section: A Hallmarks Of the Htllmentioning
confidence: 99%
“…al. [19] e para uma boa aproximação, a modulação pode ser representada por um harmônico simples (função senoidal).…”
Section: Interação Com Modulaçãounclassified