Resonant-Cavity GeSn Photodiode for Low-Noise SWIR Detection
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Solution Overview
Problem
Current single-photon detectors, particularly in the short-wave infrared (SWIR) regime, face challenges such as low sensitivity, high noise, and compatibility issues with existing Si CMOS technology, limiting their application in advanced communication systems and sensing applications.
Innovation Solution
A CMOS-compatible resonant-cavity-enhanced (RCE) photodiode detector using a GeSn absorption layer within an optical cavity, enhancing absorption efficiency and reducing noise by optimizing the GeSn layer's thickness and Sn content, allowing for high-performance single-photon detection at 1550 nm and 2000 nm wavelengths.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Adaptability or versatility
If Ge-on-Si SPAD is used to extend detection wavelength beyond 1000 nm, then spectral coverage is improved, but absorption efficiency deteriorates due to low absorption coefficient
Solution Approach 1:
The patent introduces an optical cavity dimension to enhance light absorption. By creating a resonant cavity structure with specific length and refractive index conditions, the light is confined and reflected multiple times through the Ge absorption layer, effectively increasing the interaction path length without increasing the physical thickness of the layer. This resolves the contradiction by adding an optical dimension rather than simply increasing material thickness.
Solution Approach 2:
The patent employs a composite structure combining Ge absorption layer with optical cavity components (mirrors, dielectric layers). This composite design leverages the high absorption coefficient of Ge at specific wavelengths while using the optical cavity to compensate for the low absorption at other wavelengths, achieving both extended spectral coverage and maintained absorption efficiency.
2Adaptability or versatility
If GeSn absorption layer is used to achieve detection at 2000 nm, then spectral coverage is improved, but manufacturing complexity increases due to material compatibility challenges
Solution Approach 1:
The patent systematically varies the Sn content in the GeSn alloy to precisely control the detection wavelength. By adjusting the Sn concentration parameter, the bandgap and absorption characteristics are tuned to match specific wavelength requirements (1550 nm, 2000 nm), enabling flexible spectral coverage while maintaining compatibility with existing semiconductor manufacturing processes.
Solution Approach 2:
The GeSn-based optical cavity detector serves multiple functions: it provides extended spectral coverage up to 2000 nm, maintains compatibility with CMOS fabrication processes, and achieves high absorption efficiency through the optical cavity enhancement. This multi-functional design reduces overall system complexity by integrating multiple capabilities into a single device structure.
3Reliability
If absorption layer thickness is increased to improve absorption efficiency, then absorption efficiency is improved, but noise increases due to higher dark count rate
Solution Approach 1:
Instead of increasing the physical thickness of the absorption layer, the patent introduces an optical cavity dimension that creates multiple optical paths. The light is reflected back and forth through the thin absorption layer, effectively increasing the absorption probability without increasing the material thickness, thereby avoiding the associated increase in dark count rate.
Solution Approach 2:
The optical cavity acts as an intermediary structure that enhances the interaction between light and the absorption layer. By introducing mirrors and dielectric layers as intermediaries, the light is confined and redirected multiple times through the absorption layer, achieving high absorption efficiency in a thin layer without the noise penalties of thicker materials.
4Reliability
If InGaAs/InP SPAD is used for SWIR detection, then detection efficiency is improved, but compatibility with Si CMOS technology deteriorates
Solution Approach 1:
The patent uses GeSn alloys with varying Sn content to achieve detection wavelengths up to 2000 nm while maintaining lattice compatibility with Si substrates. This parameter adjustment allows the detector to achieve InGaAs/InP-level performance in the SWIR regime while remaining compatible with standard Si CMOS fabrication processes.
Solution Approach 2:
The patent creates a composite structure combining GeSn absorption layer with Si-based optical cavity components. This composite design enables SWIR detection capability comparable to InGaAs/InP devices while maintaining full compatibility with Si CMOS manufacturing, avoiding the need for complex heteroepitaxial growth processes required for III-V materials.
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
The RCE GeSn-based detector achieves high single-photon detection efficiency, low dark count rates, and compatibility with Si CMOS technology, enabling efficient detection across the SWIR regime with a thin absorption layer, thus addressing the limitations of existing detectors.
Implementation Method 1
a GeSn absorption layer; wherein the GeSn absorption layer is disposed within the optical cavity and arranged between the overlying light-receiving portion and the underlying mirror, and the overlying light-receiving portion is configured to receive light to be detected by the photodiode detector
Implementation Method 2
CMOS-compatible resonant-cavity-enhanced (RCE) photodiode detector using a GeSn absorption layer within an optical cavity, enhancing absorption efficiency
Data Source
AI summary
According to embodiments of the present invention, a photodiode detector is provided. The photodiode detector includes an optical cavity including an overlying light-receiving portion and an underlying minor; and a GeSn absorption layer. The GeSn absorption layer may be disposed within the optical cavity and arranged between the overlying light-receiving portion and the underlying mirror. The overlying light-receiving portion may be configured to receive light to be detected by the photodiode detector. According to further embodiments of the present invention, a method of fabricating a photodiode detector is also provided.


