Home > Research > Publications & Outputs > Spin-orbit coupling and broken spin degeneracy ...

Electronic data

  • Mccann spinorbit PRB2010

    Rights statement: © 2010 The American Physical Society

    Final published version, 163 KB, PDF document

Links

Text available via DOI:

Keywords

View graph of relations

Spin-orbit coupling and broken spin degeneracy in multilayer graphene

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Published

Standard

Spin-orbit coupling and broken spin degeneracy in multilayer graphene. / McCann, Edward; Koshino, Mikito.
In: Physical review B, Vol. 81, No. 24, 241409, 15.06.2010.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

APA

Vancouver

McCann E, Koshino M. Spin-orbit coupling and broken spin degeneracy in multilayer graphene. Physical review B. 2010 Jun 15;81(24):241409. doi: 10.1103/PhysRevB.81.241409

Author

McCann, Edward ; Koshino, Mikito. / Spin-orbit coupling and broken spin degeneracy in multilayer graphene. In: Physical review B. 2010 ; Vol. 81, No. 24.

Bibtex

@article{30509320006f44aca6caed0c2484d8e3,
title = "Spin-orbit coupling and broken spin degeneracy in multilayer graphene",
abstract = "Since the lattices of ABA-stacked graphene multilayers with an even number of layers, as well as that of monolayer graphene, satisfy spatial-inversion symmetry, their electronic bands must be spin degenerate in the presence of time-inversion symmetry. In intrinsic monolayer and bilayer graphene, when symmetry is not broken by external fields, the only spin-orbit coupling present at low energy near the corner of the Brillouin zone is the Kane-Mele term, that opens a bulk energy gap but does not break the spin degeneracy of the energy bands [C. L. Kane and E. J. Mele, Phys. Rev. Lett. 95, 226801 (2005)]. However, spin splitting is allowed in multilayers with an odd number of layers because their lattices do not satisfy spatial-inversion symmetry. We show that, in trilayer graphene, in addition to the Kane-Mele term, there is a second type of intrinsic spin-orbit coupling present at low energy near the corner of the Brillouin zone. It introduces a Zeeman-type spin splitting of the energy bands at each valley with an opposite sign of the effective magnetic field in the two valleys. We estimate the magnitude of the effective field to be ~2 T.",
keywords = "graphene",
author = "Edward McCann and Mikito Koshino",
note = "{\textcopyright} 2010 The American Physical Society",
year = "2010",
month = jun,
day = "15",
doi = "10.1103/PhysRevB.81.241409",
language = "English",
volume = "81",
journal = "Physical review B",
issn = "1550-235X",
publisher = "AMER PHYSICAL SOC",
number = "24",

}

RIS

TY - JOUR

T1 - Spin-orbit coupling and broken spin degeneracy in multilayer graphene

AU - McCann, Edward

AU - Koshino, Mikito

N1 - © 2010 The American Physical Society

PY - 2010/6/15

Y1 - 2010/6/15

N2 - Since the lattices of ABA-stacked graphene multilayers with an even number of layers, as well as that of monolayer graphene, satisfy spatial-inversion symmetry, their electronic bands must be spin degenerate in the presence of time-inversion symmetry. In intrinsic monolayer and bilayer graphene, when symmetry is not broken by external fields, the only spin-orbit coupling present at low energy near the corner of the Brillouin zone is the Kane-Mele term, that opens a bulk energy gap but does not break the spin degeneracy of the energy bands [C. L. Kane and E. J. Mele, Phys. Rev. Lett. 95, 226801 (2005)]. However, spin splitting is allowed in multilayers with an odd number of layers because their lattices do not satisfy spatial-inversion symmetry. We show that, in trilayer graphene, in addition to the Kane-Mele term, there is a second type of intrinsic spin-orbit coupling present at low energy near the corner of the Brillouin zone. It introduces a Zeeman-type spin splitting of the energy bands at each valley with an opposite sign of the effective magnetic field in the two valleys. We estimate the magnitude of the effective field to be ~2 T.

AB - Since the lattices of ABA-stacked graphene multilayers with an even number of layers, as well as that of monolayer graphene, satisfy spatial-inversion symmetry, their electronic bands must be spin degenerate in the presence of time-inversion symmetry. In intrinsic monolayer and bilayer graphene, when symmetry is not broken by external fields, the only spin-orbit coupling present at low energy near the corner of the Brillouin zone is the Kane-Mele term, that opens a bulk energy gap but does not break the spin degeneracy of the energy bands [C. L. Kane and E. J. Mele, Phys. Rev. Lett. 95, 226801 (2005)]. However, spin splitting is allowed in multilayers with an odd number of layers because their lattices do not satisfy spatial-inversion symmetry. We show that, in trilayer graphene, in addition to the Kane-Mele term, there is a second type of intrinsic spin-orbit coupling present at low energy near the corner of the Brillouin zone. It introduces a Zeeman-type spin splitting of the energy bands at each valley with an opposite sign of the effective magnetic field in the two valleys. We estimate the magnitude of the effective field to be ~2 T.

KW - graphene

U2 - 10.1103/PhysRevB.81.241409

DO - 10.1103/PhysRevB.81.241409

M3 - Journal article

VL - 81

JO - Physical review B

JF - Physical review B

SN - 1550-235X

IS - 24

M1 - 241409

ER -