Non-Hermitian Floquet Phases with Even-Integer Topological Invariants in a Periodically Quenched Two-Leg Ladder

Periodically driven non-Hermitian systems could possess exotic nonequilibrium phases with unique topological, dynamical, and transport properties. In this work, we introduce an experimentally realizable two-leg ladder model subjecting to both time-periodic quenches and non-Hermitian effects, which b...

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Main Author: Longwen Zhou
Format: Article
Language:English
Published: MDPI AG 2020-07-01
Series:Entropy
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Online Access:https://www.mdpi.com/1099-4300/22/7/746
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spelling doaj-798e8599b2f449668fd46c037aa78adc2020-11-25T03:07:18ZengMDPI AGEntropy1099-43002020-07-012274674610.3390/e22070746Non-Hermitian Floquet Phases with Even-Integer Topological Invariants in a Periodically Quenched Two-Leg LadderLongwen Zhou0Department of Physics, College of Information Science and Engineering, Ocean University of China, Qingdao 266100, ChinaPeriodically driven non-Hermitian systems could possess exotic nonequilibrium phases with unique topological, dynamical, and transport properties. In this work, we introduce an experimentally realizable two-leg ladder model subjecting to both time-periodic quenches and non-Hermitian effects, which belongs to an extended CII symmetry class. Due to the interplay between drivings and nonreciprocity, rich non-Hermitian Floquet topological phases emerge in the system, with each of them characterized by a pair of even-integer topological invariants <inline-formula> <math display="inline"> <semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>w</mi> <mn>0</mn> </msub> <mo>,</mo> <msub> <mi>w</mi> <mi>π</mi> </msub> <mo stretchy="false">)</mo> <mo>∈</mo> <mn>2</mn> <mi mathvariant="double-struck">Z</mi> <mo>×</mo> <mn>2</mn> <mi mathvariant="double-struck">Z</mi> </mrow> </semantics> </math> </inline-formula>. Under the open boundary condition, these invariants further predict the number of zero- and <inline-formula> <math display="inline"> <semantics> <mi>π</mi> </semantics> </math> </inline-formula>-quasienergy modes localized around the edges of the system. We finally construct a generalized version of the mean chiral displacement, which could be employed as a dynamical probe to the topological invariants of non-Hermitian Floquet phases in the CII symmetry class. Our work thus introduces a new type of non-Hermitian Floquet topological matter, and further reveals the richness of topology and dynamics in driven open systems.https://www.mdpi.com/1099-4300/22/7/746non-hermitian systemfloquet systemtopological phasedynamics
collection DOAJ
language English
format Article
sources DOAJ
author Longwen Zhou
spellingShingle Longwen Zhou
Non-Hermitian Floquet Phases with Even-Integer Topological Invariants in a Periodically Quenched Two-Leg Ladder
Entropy
non-hermitian system
floquet system
topological phase
dynamics
author_facet Longwen Zhou
author_sort Longwen Zhou
title Non-Hermitian Floquet Phases with Even-Integer Topological Invariants in a Periodically Quenched Two-Leg Ladder
title_short Non-Hermitian Floquet Phases with Even-Integer Topological Invariants in a Periodically Quenched Two-Leg Ladder
title_full Non-Hermitian Floquet Phases with Even-Integer Topological Invariants in a Periodically Quenched Two-Leg Ladder
title_fullStr Non-Hermitian Floquet Phases with Even-Integer Topological Invariants in a Periodically Quenched Two-Leg Ladder
title_full_unstemmed Non-Hermitian Floquet Phases with Even-Integer Topological Invariants in a Periodically Quenched Two-Leg Ladder
title_sort non-hermitian floquet phases with even-integer topological invariants in a periodically quenched two-leg ladder
publisher MDPI AG
series Entropy
issn 1099-4300
publishDate 2020-07-01
description Periodically driven non-Hermitian systems could possess exotic nonequilibrium phases with unique topological, dynamical, and transport properties. In this work, we introduce an experimentally realizable two-leg ladder model subjecting to both time-periodic quenches and non-Hermitian effects, which belongs to an extended CII symmetry class. Due to the interplay between drivings and nonreciprocity, rich non-Hermitian Floquet topological phases emerge in the system, with each of them characterized by a pair of even-integer topological invariants <inline-formula> <math display="inline"> <semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>w</mi> <mn>0</mn> </msub> <mo>,</mo> <msub> <mi>w</mi> <mi>π</mi> </msub> <mo stretchy="false">)</mo> <mo>∈</mo> <mn>2</mn> <mi mathvariant="double-struck">Z</mi> <mo>×</mo> <mn>2</mn> <mi mathvariant="double-struck">Z</mi> </mrow> </semantics> </math> </inline-formula>. Under the open boundary condition, these invariants further predict the number of zero- and <inline-formula> <math display="inline"> <semantics> <mi>π</mi> </semantics> </math> </inline-formula>-quasienergy modes localized around the edges of the system. We finally construct a generalized version of the mean chiral displacement, which could be employed as a dynamical probe to the topological invariants of non-Hermitian Floquet phases in the CII symmetry class. Our work thus introduces a new type of non-Hermitian Floquet topological matter, and further reveals the richness of topology and dynamics in driven open systems.
topic non-hermitian system
floquet system
topological phase
dynamics
url https://www.mdpi.com/1099-4300/22/7/746
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