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Polarization Splitting at Visible Wavelengths with the Rutile TiO(2) Ridge Waveguide

On-chip polarization control is in high demand for novel integrated photonic applications such as polarization division multiplexing and quantum communications. However, due to the sensitive scaling of the device dimension with wavelength and the visible-light absorption properties, traditional pass...

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Detalles Bibliográficos
Autores principales: Zheng, Xinzhi, Ma, Yujie, Zhao, Chenxi, Xiang, Bingxi, Yu, Mingyang, Dai, Yanmeng, Xu, Fang, Lv, Jinman, Lu, Fei, Zhou, Cangtao, Ruan, Shuangchen
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10300929/
https://www.ncbi.nlm.nih.gov/pubmed/37368321
http://dx.doi.org/10.3390/nano13121891
Descripción
Sumario:On-chip polarization control is in high demand for novel integrated photonic applications such as polarization division multiplexing and quantum communications. However, due to the sensitive scaling of the device dimension with wavelength and the visible-light absorption properties, traditional passive silicon photonic devices with asymmetric waveguide structures cannot achieve polarization control at visible wavelengths. In this paper, a new polarization-splitting mechanism based on energy distributions of the fundamental polarized modes in the r-TiO(2) ridge waveguide is investigated. The bending loss for different bending radii and the optical coupling properties of the fundamental modes in different r-TiO(2) ridge waveguide configurations are analyzed. In particular, a polarization splitter with a high extinction ratio operating at visible wavelengths based on directional couplers (DCs) in the r-TiO(2) ridge waveguide is proposed. Polarization-selective filters based on micro-ring resonators (MRRs) with resonances of only TE or TM polarizations are designed and operated. Our results show that polarization-splitters for visible wavelengths with a high extinction ratio in DC or MRR configurations can be achieved with a simple r-TiO(2) ridge waveguide structure.