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Majorana Bound States without Vortices in Topological Superconductors with Electrostatic Defects

Source: Phys. Rev. Lett. 105, 046803 (2010); doi:10.1103/PhysRevLett.105.046803

Published 21 July 2010

PACS
  • 73.20.At
    Surface states, band structure, electron density of states
  • 73.20.Hb
    Surface impurity and defect levels; energy states of adsorbed species
  • 74.20.-z
    Theories and models of superconducting state
  • 74.25.fc
    Electric and thermal conductivity
  • YEAR: 2010
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
M. Wimmer,1 A. R. Akhmerov,1 M. V. Medvedyeva,1 J. Tworzydlo,2 and C. W. J. Beenakker1
1Instituut-Lorentz, Universiteit Leiden, P.O. Box 9506, 2300 RA Leiden, The Netherlands
2Institute of Theoretical Physics, University of Warsaw, Hoza 69, 00-681 Warsaw, Poland

Vortices in two-dimensional superconductors with broken time-reversal and spin-rotation symmetry can bind states at zero excitation energy. These so-called Majorana bound states transform a thermal insulator into a thermal metal and may be used to encode topologically protected qubits. We identify an alternative mechanism for the formation of Majorana bound states, akin to the way in which Shockley states are formed on metal surfaces: An electrostatic line defect can have a pair of Majorana bound states at the end points. The Shockley mechanism explains the appearance of a thermal metal in vortex-free lattice models of chiral p-wave superconductors and (unlike the vortex mechanism) is also operative in the topologically trivial phase. ©2010 The American Physical Society
History: Received 18 February 2010; published 21 July 2010
Permalink: http://link.aps.org/abstract/PRL/v105/e046803
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