Planar chiral metasurfaces with maximal and tunable chiroptical response driven by bound states in the continuum.


Journal

Nature communications
ISSN: 2041-1723
Titre abrégé: Nat Commun
Pays: England
ID NLM: 101528555

Informations de publication

Date de publication:
15 Jul 2022
Historique:
received: 22 12 2021
accepted: 06 07 2022
entrez: 15 7 2022
pubmed: 16 7 2022
medline: 16 7 2022
Statut: epublish

Résumé

Optical metasurfaces with high quality factors (Q-factors) of chiral resonances can boost substantially light-matter interaction for various applications of chiral response in ultrathin, active, and nonlinear metadevices. However, current approaches lack the flexibility to enhance and tune the chirality and Q-factor simultaneously. Here, we suggest a design of chiral metasurface supporting bound state in the continuum (BIC) and demonstrate experimentally chiroptical responses with ultra-high Q-factors and near-perfect circular dichroism (CD = 0.93) at optical frequencies. We employ the symmetry-reduced meta-atoms with high birefringence supporting winding elliptical eigenstate polarizations with opposite helicity. It provides a convenient way for achieving the maximal planar chirality tuned by either breaking in-plane structure symmetry or changing illumination angle. Beyond linear CD, we also achieved strong near-field enhancement CD and near-unitary nonlinear CD in the same planar chiral metasurface design with circular eigen-polarization. Sharply resonant chirality realized in planar metasurfaces promises various practical applications including chiral lasers and chiral nonlinear filters.

Identifiants

pubmed: 35840567
doi: 10.1038/s41467-022-31877-1
pii: 10.1038/s41467-022-31877-1
pmc: PMC9287326
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

4111

Informations de copyright

© 2022. The Author(s).

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Auteurs

Tan Shi (T)

Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Institute of Photonics Technology, Jinan University, 510632, Guangzhou, China.

Zi-Lan Deng (ZL)

Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Institute of Photonics Technology, Jinan University, 510632, Guangzhou, China. zilandeng@jnu.edu.cn.

Guangzhou Geng (G)

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, 100191, Beijing, China.

Xianzhi Zeng (X)

Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Institute of Photonics Technology, Jinan University, 510632, Guangzhou, China.

Yixuan Zeng (Y)

School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore.

Guangwei Hu (G)

School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore.

Adam Overvig (A)

Photonics Initiative, Advanced Science Research Center, City University of New York, New York, NY, 10031, USA.

Junjie Li (J)

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, 100191, Beijing, China. jjli@iphy.ac.cn.

Cheng-Wei Qiu (CW)

Department of Electrical and Computer Engineering, National University of Singapore, Kent Ridge, 117583, Republic of Singapore.

Andrea Alù (A)

Photonics Initiative, Advanced Science Research Center, City University of New York, New York, NY, 10031, USA.

Yuri S Kivshar (YS)

Nonlinear Physics Center, Research School of Physics, Australian National University, Canberra, ACT, 2601, Australia.

Xiangping Li (X)

Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Institute of Photonics Technology, Jinan University, 510632, Guangzhou, China. xiangpingli@jnu.edu.cn.

Classifications MeSH