Majorana bound states in two-channel time-reversal-symmetric nanowire systems

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Standard

Majorana bound states in two-channel time-reversal-symmetric nanowire systems. / Gaidamauskas, Erikas; Paaske, Jens; Flensberg, Karsten.

I: Physical Review Letters, Bind 112, Nr. 12, 126402, 25.03.2014.

Publikation: Bidrag til tidsskriftTidsskriftartikelForskningfagfællebedømt

Harvard

Gaidamauskas, E, Paaske, J & Flensberg, K 2014, 'Majorana bound states in two-channel time-reversal-symmetric nanowire systems', Physical Review Letters, bind 112, nr. 12, 126402. https://doi.org/10.1103/PhysRevLett.112.126402

APA

Gaidamauskas, E., Paaske, J., & Flensberg, K. (2014). Majorana bound states in two-channel time-reversal-symmetric nanowire systems. Physical Review Letters, 112(12), [126402]. https://doi.org/10.1103/PhysRevLett.112.126402

Vancouver

Gaidamauskas E, Paaske J, Flensberg K. Majorana bound states in two-channel time-reversal-symmetric nanowire systems. Physical Review Letters. 2014 mar. 25;112(12). 126402. https://doi.org/10.1103/PhysRevLett.112.126402

Author

Gaidamauskas, Erikas ; Paaske, Jens ; Flensberg, Karsten. / Majorana bound states in two-channel time-reversal-symmetric nanowire systems. I: Physical Review Letters. 2014 ; Bind 112, Nr. 12.

Bibtex

@article{db858fee426b456dae760b086500d754,
title = "Majorana bound states in two-channel time-reversal-symmetric nanowire systems",
abstract = "We consider time-reversal-symmetric two-channel semiconducting quantum wires proximity coupled to a conventional s-wave superconductor. We analyze the requirements for a non-trivial topological phase, and find that necessary conditions are 1) the determinant of the pairing matrix in channel space must be negative, 2) inversion symmetry must be broken, and 3) the two channels must have different spin-orbit couplings. For the case of collinear spin-orbit directions, we find a general expression for the topological invariant by block diagonalization into two blocks with chiral symmetry only. By projection to the low-energy sector we solve for the zero modes explicitly and study the details of the gap closing, which in the general case happens at finite momenta.",
keywords = "cond-mat.mes-hall, cond-mat.supr-con",
author = "Erikas Gaidamauskas and Jens Paaske and Karsten Flensberg",
year = "2014",
month = mar,
day = "25",
doi = "10.1103/PhysRevLett.112.126402",
language = "English",
volume = "112",
journal = "Physical Review Letters",
issn = "0031-9007",
publisher = "American Physical Society",
number = "12",

}

RIS

TY - JOUR

T1 - Majorana bound states in two-channel time-reversal-symmetric nanowire systems

AU - Gaidamauskas, Erikas

AU - Paaske, Jens

AU - Flensberg, Karsten

PY - 2014/3/25

Y1 - 2014/3/25

N2 - We consider time-reversal-symmetric two-channel semiconducting quantum wires proximity coupled to a conventional s-wave superconductor. We analyze the requirements for a non-trivial topological phase, and find that necessary conditions are 1) the determinant of the pairing matrix in channel space must be negative, 2) inversion symmetry must be broken, and 3) the two channels must have different spin-orbit couplings. For the case of collinear spin-orbit directions, we find a general expression for the topological invariant by block diagonalization into two blocks with chiral symmetry only. By projection to the low-energy sector we solve for the zero modes explicitly and study the details of the gap closing, which in the general case happens at finite momenta.

AB - We consider time-reversal-symmetric two-channel semiconducting quantum wires proximity coupled to a conventional s-wave superconductor. We analyze the requirements for a non-trivial topological phase, and find that necessary conditions are 1) the determinant of the pairing matrix in channel space must be negative, 2) inversion symmetry must be broken, and 3) the two channels must have different spin-orbit couplings. For the case of collinear spin-orbit directions, we find a general expression for the topological invariant by block diagonalization into two blocks with chiral symmetry only. By projection to the low-energy sector we solve for the zero modes explicitly and study the details of the gap closing, which in the general case happens at finite momenta.

KW - cond-mat.mes-hall

KW - cond-mat.supr-con

U2 - 10.1103/PhysRevLett.112.126402

DO - 10.1103/PhysRevLett.112.126402

M3 - Journal article

VL - 112

JO - Physical Review Letters

JF - Physical Review Letters

SN - 0031-9007

IS - 12

M1 - 126402

ER -

ID: 50797558