Quantized transport and steady states of Floquet topological insulators

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Quantized transport and steady states of Floquet topological insulators. / Esin, Iliya; Rudner, Mark S.; Refael, Gil; Lindner, Netanel H.

In: Physical Review B, Vol. 97, No. 24, 245401, 06.06.2018.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Esin, I, Rudner, MS, Refael, G & Lindner, NH 2018, 'Quantized transport and steady states of Floquet topological insulators', Physical Review B, vol. 97, no. 24, 245401. https://doi.org/10.1103/PhysRevB.97.245401

APA

Esin, I., Rudner, M. S., Refael, G., & Lindner, N. H. (2018). Quantized transport and steady states of Floquet topological insulators. Physical Review B, 97(24), [245401]. https://doi.org/10.1103/PhysRevB.97.245401

Vancouver

Esin I, Rudner MS, Refael G, Lindner NH. Quantized transport and steady states of Floquet topological insulators. Physical Review B. 2018 Jun 6;97(24). 245401. https://doi.org/10.1103/PhysRevB.97.245401

Author

Esin, Iliya ; Rudner, Mark S. ; Refael, Gil ; Lindner, Netanel H. / Quantized transport and steady states of Floquet topological insulators. In: Physical Review B. 2018 ; Vol. 97, No. 24.

Bibtex

@article{de1fb5ac0d7e4e7db241fca4c6b4c1b9,
title = "Quantized transport and steady states of Floquet topological insulators",
abstract = "Robust electronic edge or surface modes play key roles in the fascinating quantized responses exhibited by topological materials. Even in trivial materials, topological bands and edge states can be induced dynamically by a time-periodic drive. Such Floquet topological insulators (FTIs) inherently exist out of equilibrium; the extent to which they can host quantized transport, which depends on the steady-state population of their dynamically induced edge states, remains a crucial question. In this work, we obtain the steady states of two-dimensional FTIs in the presence of the natural dissipation mechanisms present in solid state systems. We give conditions under which the steady-state distribution resembles that of a topological insulator in the Floquet basis. In this state, the distribution in the Floquet edge modes exhibits a sharp feature akin to a Fermi level, while the bulk hosts a small density of excitations. We determine the regimes where topological edge-state transport persists and can be observed in FTIs.",
author = "Iliya Esin and Rudner, {Mark S.} and Gil Refael and Lindner, {Netanel H.}",
note = "[Qdev]",
year = "2018",
month = jun,
day = "6",
doi = "10.1103/PhysRevB.97.245401",
language = "English",
volume = "97",
journal = "Physical Review B",
issn = "2469-9950",
publisher = "American Physical Society",
number = "24",

}

RIS

TY - JOUR

T1 - Quantized transport and steady states of Floquet topological insulators

AU - Esin, Iliya

AU - Rudner, Mark S.

AU - Refael, Gil

AU - Lindner, Netanel H.

N1 - [Qdev]

PY - 2018/6/6

Y1 - 2018/6/6

N2 - Robust electronic edge or surface modes play key roles in the fascinating quantized responses exhibited by topological materials. Even in trivial materials, topological bands and edge states can be induced dynamically by a time-periodic drive. Such Floquet topological insulators (FTIs) inherently exist out of equilibrium; the extent to which they can host quantized transport, which depends on the steady-state population of their dynamically induced edge states, remains a crucial question. In this work, we obtain the steady states of two-dimensional FTIs in the presence of the natural dissipation mechanisms present in solid state systems. We give conditions under which the steady-state distribution resembles that of a topological insulator in the Floquet basis. In this state, the distribution in the Floquet edge modes exhibits a sharp feature akin to a Fermi level, while the bulk hosts a small density of excitations. We determine the regimes where topological edge-state transport persists and can be observed in FTIs.

AB - Robust electronic edge or surface modes play key roles in the fascinating quantized responses exhibited by topological materials. Even in trivial materials, topological bands and edge states can be induced dynamically by a time-periodic drive. Such Floquet topological insulators (FTIs) inherently exist out of equilibrium; the extent to which they can host quantized transport, which depends on the steady-state population of their dynamically induced edge states, remains a crucial question. In this work, we obtain the steady states of two-dimensional FTIs in the presence of the natural dissipation mechanisms present in solid state systems. We give conditions under which the steady-state distribution resembles that of a topological insulator in the Floquet basis. In this state, the distribution in the Floquet edge modes exhibits a sharp feature akin to a Fermi level, while the bulk hosts a small density of excitations. We determine the regimes where topological edge-state transport persists and can be observed in FTIs.

U2 - 10.1103/PhysRevB.97.245401

DO - 10.1103/PhysRevB.97.245401

M3 - Journal article

AN - SCOPUS:85048358616

VL - 97

JO - Physical Review B

JF - Physical Review B

SN - 2469-9950

IS - 24

M1 - 245401

ER -

ID: 198614001