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利用电可调极化激元超表面实现宽带巨非线性响应

Broadband giant nonlinear response using electrically tunable polaritonic metasurfaces.

作者信息

Yu Jaeyeon, Park Seongjin, Hwang Inyong, Boehm Gerhard, Belkin Mikhail A, Lee Jongwon

机构信息

Department of Electrical Engineering, Ulsan National Institute of Science and Technology, Ulsan, 44919, Republic of Korea.

Walter Schottky Institute, Technical University of Munich, Am Coulombwall 4, 85748 Garching, Germany.

出版信息

Nanophotonics. 2024 Jan 9;13(7):1131-1139. doi: 10.1515/nanoph-2023-0682. eCollection 2024 Mar.

DOI:10.1515/nanoph-2023-0682
PMID:39634010
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11502031/
Abstract

Intersubband transitions in semiconductor heterostructures offer a way to achieve large and designable nonlinearities with dynamic modulation of intersubband energies through the Stark effect. One promising approach for incorporating these nonlinearities into free space optics is a nonlinear polaritonic metasurface, which derives resonant coupling between intersubband nonlinearities and optical modes in nanocavities. Recent work has shown efficient frequency mixing at low pumping intensities, with the ability to electrically tune the phase, amplitude, and spectral peak of it. However, the spectral tunability of intersubband nonlinearities is constrained by the static spectral response of nanocavities. To overcome this limitation, we present nonlinear polaritonic metasurfaces for a broadband giant nonlinear response. This is achieved by combining a Stark tunable nonlinear response from a quantum-engineered semi-conductor heterostructure with arrays of three nanocavities with different resonant wavelengths. We experimentally demonstrate broadband second harmonic generation (SHG) and a shift in the peak SHG efficiency within the range of 8.9-10.6 μm by applying bias voltage. This work will provide a promising route for achieving broadband and electrically tunable nonlinearities in metasurfaces.

摘要

半导体异质结构中的子带间跃迁提供了一种途径,可通过斯塔克效应动态调制子带间能量来实现大的且可设计的非线性。将这些非线性纳入自由空间光学的一种有前景的方法是一种非线性极化激元超表面,它在纳米腔中实现子带间非线性与光学模式之间的共振耦合。最近的研究表明,在低泵浦强度下能实现高效的频率混合,并且能够对其相位、幅度和光谱峰值进行电调谐。然而,子带间非线性的光谱可调性受到纳米腔静态光谱响应的限制。为了克服这一限制,我们展示了用于宽带巨非线性响应的非线性极化激元超表面。这是通过将量子工程半导体异质结构的斯塔克可调非线性响应与具有不同共振波长的三个纳米腔阵列相结合来实现的。我们通过施加偏置电压,实验证明了宽带二次谐波产生(SHG)以及在8.9 - 10.6μm范围内SHG峰值效率的移动。这项工作将为在超表面中实现宽带和电可调非线性提供一条有前景的途径。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/b42bf8ab643f/j_nanoph-2023-0682_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/cf9b96787590/j_nanoph-2023-0682_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/5c0fdfdd55b0/j_nanoph-2023-0682_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/2730e2733376/j_nanoph-2023-0682_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/b42bf8ab643f/j_nanoph-2023-0682_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/cf9b96787590/j_nanoph-2023-0682_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/5c0fdfdd55b0/j_nanoph-2023-0682_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/2730e2733376/j_nanoph-2023-0682_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6dee/11502031/b42bf8ab643f/j_nanoph-2023-0682_fig_004.jpg

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本文引用的文献

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