2018
DOI: 10.1103/physrevb.97.085420
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Perfect valley filter based on a topological phase in a disordered Sb monolayer heterostructure

Abstract: The hydrogenated Sb monolayer epitaxially grown on a LaFeO3 substrate is a novel type of two-dimensional material hosting quantum spin-quantum anomalous Hall (QS-QAH) states. For a device formed by Sb monolayer ribbon, the QAH edge states, belong to a single valley, are located at opposite edges of the ribbon. The QSH edge states, on the other hand, belong to the other valley and are distributed in a very narrow region at the same edge. In this paper, we find such material can be used to fabricate perfect vall… Show more

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Cited by 23 publications
(18 citation statements)
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“…Moreover, the original Dirac cones at the K and K’ points are opened to form a complete photonic bandgap, resulting in the edge states at the interfaces of different valley Hall phases [ 23 , 24 , 25 ], which are immune to backscattering [ 28 , 29 ] caused by defects and acute light channels. In recent years, valley topological insulators (TIs) have been widely studied in optical, acoustic, and electronic systems, such as valley topological robust transport [ 18 , 19 , 20 ], topological photon routing [ 24 , 30 ], unidirectional light transport [ 24 ], valley topological edge state frequency tuning [ 13 ], valley topological acoustic wave group velocity modulation based on phononic crystals [ 13 ], and topological spin–valley filtering effects [ 31 , 32 ]. These studies have opened up unprecedented application opportunities for valley TIs in the fields of tunable acoustics, topological photonics, and the emerging field of nontrivial states.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, the original Dirac cones at the K and K’ points are opened to form a complete photonic bandgap, resulting in the edge states at the interfaces of different valley Hall phases [ 23 , 24 , 25 ], which are immune to backscattering [ 28 , 29 ] caused by defects and acute light channels. In recent years, valley topological insulators (TIs) have been widely studied in optical, acoustic, and electronic systems, such as valley topological robust transport [ 18 , 19 , 20 ], topological photon routing [ 24 , 30 ], unidirectional light transport [ 24 ], valley topological edge state frequency tuning [ 13 ], valley topological acoustic wave group velocity modulation based on phononic crystals [ 13 ], and topological spin–valley filtering effects [ 31 , 32 ]. These studies have opened up unprecedented application opportunities for valley TIs in the fields of tunable acoustics, topological photonics, and the emerging field of nontrivial states.…”
Section: Introductionmentioning
confidence: 99%
“…Like the spin degree of freedom in spintronics devices [9][10][11], these inequivalent valleys or the valley degrees of freedom can also be used as information carriers to give birth to valleytronics [8,12,13]. Many unique transport phenomena can be realized by regulating these two degrees of freedom, such as fully spin-polarized current, the valley filter [14], and spin-valley filter [15][16][17][18][19].…”
Section: Introductionmentioning
confidence: 99%
“…However, the weak spin-orbit coupling of these systems only leads to a tiny bulk gap with the order of a few meV, which limits the applications in the topological devices. Recently, the QSH effect is proposed in group-V monolayers (e.g., bismuthene [17][18][19][20] and antimonene [21][22][23][24] ). In these systems, the bulk gap can reach the same order of the atomic spin-orbit coupling strength of Bi and Sb.…”
Section: Introductionmentioning
confidence: 99%