A one-dimensional boundary of a two-dimensional topological superconductor can host a number of topo-logically protected chiral modes. Combining two topological superconductors with different topological indices, it is possible to achieve a situation when only a given number of channels (m) are topologically protected, while others are not and therefore are subject to Anderson localization in the presence of disorder. We study transport properties of such quasi-one-dimensional quantum wires with broken time-reversal and spin-rotational symmetries (class D) and calculate the average conductance, its variance and the third cumulant, as well as the average shot noise power. The results are obtained for arbitrary wire length, tracing a crossover from the diffusive Drude regime to the regime of strong localization where only m protected channels conduct. Our approach is based on the nonperturbative treatment of the nonlinear supersymmetric sigma model of symmetry class D with two replicas developed in our recent publication [D. S. Antonenko et al., Phys. Rev. B 102, 195152 (2020)]. The presence of topologically protected modes results in the appearance of a topological Wess-Zumino-Witten term in the sigma-model action, which leads to an additional subsidiary series of eigenstates of the transfer-matrix Hamiltonian. The developed formalism can be applied to study the interplay of Anderson localization and topological protection in quantum wires of other symmetry classes.
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Title
Anderson localization at the boundary of a two-dimensional topological superconductor
Publication Details
PHYSICAL REVIEW B, v 107(7), 75417
Publisher
AMER PHYSICAL SOC; COLLEGE PK
Grant note
We are grateful to E. J. K?nig for valuable discussions. This work was partially supported by the Russian Science Foundation under Grant No. 20-12-00361.
Resource Type
Journal article
Language
English
Academic Unit
Drexel University
Web of Science ID
WOS:000972005400003
Scopus ID
2-s2.0-85148331748
Other Identifier
991021861309604721
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