2013
DOI: 10.1103/physrevb.87.085425
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Generating and controlling spin-polarized currents induced by a quantum spin Hall antidot

Abstract: We study an electrically-controlled quantum spin Hall antidot embedded in a two-dimensional topological insulating bar. Helical edge states around the antidot and along the edges of the bar are tunnel-coupled. The close connection between spin and chirality, typical of helical systems, allows to generate a spin-polarized current flowing across the bar. This current is studied as a function of the external voltages, by varying the asymmetry between the barriers. For asymmetric setups, a switching behavior of th… Show more

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Cited by 38 publications
(37 citation statements)
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“…Our proposal is based on the edge states of two-dimensional (2D) topological insulators [21][22][23], whose properties are described in terms of counterpropagating channels characterized by spin-momentum locking. In the presence of interactions, these are described as helical Luttinger liquids (hLL) [24][25][26][27][28][29][30][31][32][33][34], whose first experimental manifestations have been recently observed [35]. Here, charge and spin sectors are connected and the presence of interactions implies the simultaneous fractionalization of both degrees of freedom [30,36].…”
Section: Introductionmentioning
confidence: 99%
“…Our proposal is based on the edge states of two-dimensional (2D) topological insulators [21][22][23], whose properties are described in terms of counterpropagating channels characterized by spin-momentum locking. In the presence of interactions, these are described as helical Luttinger liquids (hLL) [24][25][26][27][28][29][30][31][32][33][34], whose first experimental manifestations have been recently observed [35]. Here, charge and spin sectors are connected and the presence of interactions implies the simultaneous fractionalization of both degrees of freedom [30,36].…”
Section: Introductionmentioning
confidence: 99%
“…The number of oscillations is related to the number of particles inside the dot, as can be deduced by the first term in Eq. (24). It is worth to note that parallel and antiparallel configurations differ by half an oscillation: since the number of oscillations is related to the total charge in the dot (including the background), this reflects the fact that a fractional charge is trapped between the barriers in the antiparallel configuration, while an integer charge is trapped in the parallel configuration.…”
mentioning
confidence: 99%
“…The coupling of helical edge states to quantum dots and magnetic impurities has been addressed in several works. [28][29][30][31][32][33][34][35][36][37][38][39][40][41][42] A crucial ingredient for a net resistive…”
Section: -15mentioning
confidence: 99%