Majorana-like end states in one-dimensional dimerized Kitaev topolectrical circuit

Majorana zero modes (MZMs) have attracted tremendous attention in condensed matter and materials physics communities due to the implications in topological quantum computation. One-dimensional (1D) dimerized Kitaev chain is a prototype model for MZMs, but its realization remains a challenge in mater...

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Main Authors: Junjie Yao, Xiamin Hao, Biyu Song, Yizhen Jia, Chenqiang Hua, Miao Zhou
Format: Article
Language:English
Published: IOP Publishing 2022-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/ac6230
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author Junjie Yao
Xiamin Hao
Biyu Song
Yizhen Jia
Chenqiang Hua
Miao Zhou
author_facet Junjie Yao
Xiamin Hao
Biyu Song
Yizhen Jia
Chenqiang Hua
Miao Zhou
author_sort Junjie Yao
collection DOAJ
description Majorana zero modes (MZMs) have attracted tremendous attention in condensed matter and materials physics communities due to the implications in topological quantum computation. One-dimensional (1D) dimerized Kitaev chain is a prototype model for MZMs, but its realization remains a challenge in material systems. Here, we develop a distinctive approach to achieve Majorana-like end states (MESs) by implementing practical dimerized Kitaev topolectrical circuits. Specifically, two arrays of inductors are arranged to simulate particles and antiparticles, while intra- and inter-array capacitive connections are used to model hopping and superconducting pairing. Three topological phases can be achieved by tuning the capacitance, i.e. the trivial phase, Su–Schrieffer–Heeger topological phase and Kitaev phase, with distinct field strength distributions in real space. Majorana splitting is observed around a domain wall in the circuit, and we propose an efficient experimental observable-edge distance-to characterize the process as premonition of topological phase transition. Remarkably, dynamics of the Gaussian wave packet in time domain provide an excellent signal to detect MESs in experiments, as only MESs allow nonlocal propagation in circuit network. Our results not only manifest the superiorities of topolectrical circuits for exotic topological states, but also pave the way for possible applications in electrical engineering and signal processing.
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spelling doaj.art-c6c7a07ba7904fde8b9f7e299c8267b52023-08-09T14:23:00ZengIOP PublishingNew Journal of Physics1367-26302022-01-0124404303210.1088/1367-2630/ac6230Majorana-like end states in one-dimensional dimerized Kitaev topolectrical circuitJunjie Yao0Xiamin Hao1Biyu Song2Yizhen Jia3Chenqiang Hua4Miao Zhou5https://orcid.org/0000-0003-1390-372XSchool of Physics, Beihang University , Beijing 100191, People’s Republic of ChinaSchool of Physics, Beihang University , Beijing 100191, People’s Republic of ChinaSchool of Physics, Beihang University , Beijing 100191, People’s Republic of China; Beihang Hangzhou Innovation Institute Yuhang , Hangzhou 310023, People’s Republic of ChinaSchool of Physics, Beihang University , Beijing 100191, People’s Republic of China; Beihang Hangzhou Innovation Institute Yuhang , Hangzhou 310023, People’s Republic of ChinaBeihang Hangzhou Innovation Institute Yuhang , Hangzhou 310023, People’s Republic of ChinaSchool of Physics, Beihang University , Beijing 100191, People’s Republic of China; Beihang Hangzhou Innovation Institute Yuhang , Hangzhou 310023, People’s Republic of ChinaMajorana zero modes (MZMs) have attracted tremendous attention in condensed matter and materials physics communities due to the implications in topological quantum computation. One-dimensional (1D) dimerized Kitaev chain is a prototype model for MZMs, but its realization remains a challenge in material systems. Here, we develop a distinctive approach to achieve Majorana-like end states (MESs) by implementing practical dimerized Kitaev topolectrical circuits. Specifically, two arrays of inductors are arranged to simulate particles and antiparticles, while intra- and inter-array capacitive connections are used to model hopping and superconducting pairing. Three topological phases can be achieved by tuning the capacitance, i.e. the trivial phase, Su–Schrieffer–Heeger topological phase and Kitaev phase, with distinct field strength distributions in real space. Majorana splitting is observed around a domain wall in the circuit, and we propose an efficient experimental observable-edge distance-to characterize the process as premonition of topological phase transition. Remarkably, dynamics of the Gaussian wave packet in time domain provide an excellent signal to detect MESs in experiments, as only MESs allow nonlocal propagation in circuit network. Our results not only manifest the superiorities of topolectrical circuits for exotic topological states, but also pave the way for possible applications in electrical engineering and signal processing.https://doi.org/10.1088/1367-2630/ac6230topolectrical circuitKitaev chainband structuresMajorana splittingtopological phase transition
spellingShingle Junjie Yao
Xiamin Hao
Biyu Song
Yizhen Jia
Chenqiang Hua
Miao Zhou
Majorana-like end states in one-dimensional dimerized Kitaev topolectrical circuit
New Journal of Physics
topolectrical circuit
Kitaev chain
band structures
Majorana splitting
topological phase transition
title Majorana-like end states in one-dimensional dimerized Kitaev topolectrical circuit
title_full Majorana-like end states in one-dimensional dimerized Kitaev topolectrical circuit
title_fullStr Majorana-like end states in one-dimensional dimerized Kitaev topolectrical circuit
title_full_unstemmed Majorana-like end states in one-dimensional dimerized Kitaev topolectrical circuit
title_short Majorana-like end states in one-dimensional dimerized Kitaev topolectrical circuit
title_sort majorana like end states in one dimensional dimerized kitaev topolectrical circuit
topic topolectrical circuit
Kitaev chain
band structures
Majorana splitting
topological phase transition
url https://doi.org/10.1088/1367-2630/ac6230
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AT yizhenjia majoranalikeendstatesinonedimensionaldimerizedkitaevtopolectricalcircuit
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