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六方氮化硼纳米谐振器中连续态束缚态与极化激元的长程耦合

Bound States in the Continuum and Long-Range Coupling of Polaritons in Hexagonal Boron Nitride Nanoresonators.

作者信息

Gupta Harsh, Venturi Giacomo, Contino Tatiana, Janzen Eli, Edgar James H, De Angelis Francesco, Toma Andrea, Ambrosio Antonio, Tamagnone Michele

机构信息

Istituto Italiano di Tecnologia, Via Morego 30, 16163 Genova, Italy.

Dipartimento di Chimica e Chimica Industriale, Università Degli Studi di Genova, Via Balbi 5, 16126 Genova, Italy.

出版信息

ACS Photonics. 2024 Sep 22;11(10):4017-4026. doi: 10.1021/acsphotonics.4c00358. eCollection 2024 Oct 16.

DOI:10.1021/acsphotonics.4c00358
PMID:39429868
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11487684/
Abstract

Bound states in the continuum (BICs) garnered significant interest for their potential to create new types of nanophotonic devices. Most prior demonstrations were based on arrays of dielectric resonators, which cannot be miniaturized beyond the diffraction limit, reducing the applicability of BICs for advanced functions. Here, we demonstrate BICs and quasi-BICs based on high-quality factor phonon-polariton resonances in isotopically pure hBN and how these states can be supported by periodic arrays of nanoresonators with sizes much smaller than the wavelength. We theoretically illustrate how BICs emerge from the band structure of the arrays and verify both numerically and experimentally the presence of these states and enhanced quality factors. Furthermore, we identify and characterize simultaneously quasi-BICs and bright states. Our method can be generalized to create a large number of optical states and to tune their coupling with the environment, paving the way to miniaturized nanophotonic devices with more advanced functions.

摘要

连续统中的束缚态(BICs)因其创造新型纳米光子器件的潜力而备受关注。大多数先前的演示基于介电谐振器阵列,其无法在衍射极限之外进行小型化,这降低了BICs在高级功能方面的适用性。在此,我们展示了基于同位素纯hBN中高品质因子声子极化激元共振的BICs和准BICs,以及这些态如何由尺寸远小于波长的纳米谐振器周期阵列来支持。我们从理论上说明了BICs如何从阵列的能带结构中出现,并通过数值和实验验证了这些态的存在以及品质因子的增强。此外,我们同时识别并表征了准BICs和亮态。我们的方法可以推广到创建大量光学态并调整它们与环境的耦合,为具有更高级功能的小型化纳米光子器件铺平道路。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f1ea/11487684/e03804a0dcbd/ph4c00358_0006.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f1ea/11487684/b8f90bad5e3e/ph4c00358_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f1ea/11487684/e03804a0dcbd/ph4c00358_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f1ea/11487684/b6f712c48da8/ph4c00358_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f1ea/11487684/66cc7abc6e21/ph4c00358_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f1ea/11487684/4acd39571da8/ph4c00358_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f1ea/11487684/a53b4e5fdda8/ph4c00358_0004.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f1ea/11487684/e03804a0dcbd/ph4c00358_0006.jpg

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