Design of the Waveguide Integrated GeSn PDs on a SiN Platform in $2\,\mathrm{\mu m}$ Wavelength Band

Silicon Nitride (SiN) platform, as an integrated photonics platform compatible with CMOS technology, is increasingly competitive. However, active devices on SiN platform, such as 2<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\,\mathrm{\mu m}$</tex-math></inline-formula> wavelength band photodetector(PD), remain relatively scarce. In this work, 2<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\,\mathrm{\mu m}$</tex-math></inline-formula> wavelength band SiN waveguide GeSn PDs based on the SiN process platform were designed, including passive SiN waveguides, tapers, and GeSn PDs. The incident light's optical field propagating in the SiN waveguide couples downward into the GeSn absorption layer in the form of an evanescent wave, achieving efficient light transmission and absorption. The Maxwell's equations are solved using the finite difference method to obtain the field distribution of the electromagnetic components on the cross-section of the waveguide, determining the dimensions of the SiN waveguide and taper for single-mode transmission. Additionally, a taper structure gradually narrowing from the input end to the output end is employed to connect the waveguide above the active layer. This structure achieves a bandwidth of 75 GHz and a responsivity of 1 A/W at 2<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\,\mathrm{\mu m}$</tex-math></inline-formula> for the Ge<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${_{0.86}}$</tex-math></inline-formula>Sn<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${_{0.14}}$</tex-math></inline-formula> PD by simulation. The design of waveguide integrated GeSn PD on SiN platform provides meaningful guidance for the preparation of 2<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\,\mathrm{\mu m}$</tex-math></inline-formula> wavelength band photonic integrated circuits (PIC).

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Publication Details

Journal
IEEE Journal of Selected Topics in Quantum Electronics
Published
2024-11-08
DOI
https://doi.org/10.1109/jstqe.2024.3493913
Primary Topic
Photonic and Optical Devices
Type
article
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article

Design of the Waveguide Integrated GeSn PDs on a SiN Platform in $2\,\mathrm{\mu m}$ Wavelength Band

Jun Zheng, Mingming Li, Wanhua Zheng, Zhigang Song
IEEE Journal of Selected Topics in Quantum Electronics
Photonic and Optical Devices
article

Design of the Waveguide Integrated GeSn PDs on a SiN Platform in $2\,\mathrm{\mu m}$ Wavelength Band

Jun Zheng, Mingming Li, Wanhua Zheng, Zhigang Song
article en

Abstract

Silicon Nitride (SiN) platform, as an integrated photonics platform compatible with CMOS technology, is increasingly competitive. However, active devices on SiN platform, such as 2<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\,\mathrm{\mu m}$</tex-math></inline-formula> wavelength band photodetector(PD), remain relatively scarce. In this work, 2<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\,\mathrm{\mu m}$</tex-math></inline-formula> wavelength band SiN waveguide GeSn PDs based on the SiN process platform were designed, including passive SiN waveguides, tapers, and GeSn PDs. The incident light's optical field propagating in the SiN waveguide couples downward into the GeSn absorption layer in the form of an evanescent wave, achieving efficient light transmission and absorption. The Maxwell's equations are solved using the finite difference method to obtain the field distribution of the electromagnetic components on the cross-section of the waveguide, determining the dimensions of the SiN waveguide and taper for single-mode transmission. Additionally, a taper structure gradually narrowing from the input end to the output end is employed to connect the waveguide above the active layer. This structure achieves a bandwidth of 75 GHz and a responsivity of 1 A/W at 2<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\,\mathrm{\mu m}$</tex-math></inline-formula> for the Ge<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${_{0.86}}$</tex-math></inline-formula>Sn<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${_{0.14}}$</tex-math></inline-formula> PD by simulation. The design of waveguide integrated GeSn PD on SiN platform provides meaningful guidance for the preparation of 2<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\,\mathrm{\mu m}$</tex-math></inline-formula> wavelength band photonic integrated circuits (PIC).

IEEE Journal of Selected Topics in Quantum ElectronicsVol. 31(1: SiGeSn Infrared Photon.)
Chinese Academy of Sciences (CN), Institute of Semiconductors (CN)
Openalex Percentile: Top 82%
Photonic and Optical Devices
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