A SiGe/Si Heterojunction Phototransistor for High Sensitivity Light Detection

Silicon-based heterojunction phototransistors (HPTs) with their advantages of high internal gain, high responsivity, and compatibility with CMOS processes have attracted much attention in high-sensitivity light detection. In this article, the SiGe/Si HPT with an illuminated area of 50\times 50~\mu...

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Veröffentlicht in:IEEE transactions on electron devices 2024-11, Vol.71 (11), p.6857-6863
Hauptverfasser: Xie, Hongyun, Shen, Xiaoting, Ge, Yunpeng, Xu, Zimai, Liu, Ziming, Ma, Yudong, Na, Weicong, Jin, Dongyue, Zhang, Wanrong
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container_issue 11
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container_title IEEE transactions on electron devices
container_volume 71
creator Xie, Hongyun
Shen, Xiaoting
Ge, Yunpeng
Xu, Zimai
Liu, Ziming
Ma, Yudong
Na, Weicong
Jin, Dongyue
Zhang, Wanrong
description Silicon-based heterojunction phototransistors (HPTs) with their advantages of high internal gain, high responsivity, and compatibility with CMOS processes have attracted much attention in high-sensitivity light detection. In this article, the SiGe/Si HPT with an illuminated area of 50\times 50~\mu m2 for high responsivity and sensitivity was designed and fabricated. The optical responsivity of the fabricated SiGe/Si HPT reached 1.717 and 12.379 A/W for 405 and 650 nm, their specific detectivity values were 1.54\times 10^{{10}} and 11.16\times 10^{{10}}~\text {cm}\cdot \text {Hz}^{{0.5}}\cdot \text {W}^{-{1}} , respectively. An analytic model was developed to discuss current amplification for different wavelengths when considering absorption efficiency and carrier transportation. The emitter thickness was optimized as 60 nm to significantly improve the current amplification under short wavelengths. The achieved optical responsivity of the optimized SiGe/Si HPT for 405 and 650 nm respectively were 13.756 and 13.904 A/W, and the specific detectivity were 12.41\times 10^{{10}} and 12.54\times 10^{{10}}~\text {cm}\cdot \text {Hz}^{{0.5}} \cdot \text {W}^{-{1}} .
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In this article, the SiGe/Si HPT with an illuminated area of <inline-formula> <tex-math notation="LaTeX">50\times 50~\mu </tex-math></inline-formula>m2 for high responsivity and sensitivity was designed and fabricated. The optical responsivity of the fabricated SiGe/Si HPT reached 1.717 and 12.379 A/W for 405 and 650 nm, their specific detectivity values were <inline-formula> <tex-math notation="LaTeX">1.54\times 10^{{10}} </tex-math></inline-formula> and <inline-formula> <tex-math notation="LaTeX">11.16\times 10^{{10}}~\text {cm}\cdot \text {Hz}^{{0.5}}\cdot \text {W}^{-{1}} </tex-math></inline-formula>, respectively. An analytic model was developed to discuss current amplification for different wavelengths when considering absorption efficiency and carrier transportation. The emitter thickness was optimized as 60 nm to significantly improve the current amplification under short wavelengths. 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In this article, the SiGe/Si HPT with an illuminated area of <inline-formula> <tex-math notation="LaTeX">50\times 50~\mu </tex-math></inline-formula>m2 for high responsivity and sensitivity was designed and fabricated. The optical responsivity of the fabricated SiGe/Si HPT reached 1.717 and 12.379 A/W for 405 and 650 nm, their specific detectivity values were <inline-formula> <tex-math notation="LaTeX">1.54\times 10^{{10}} </tex-math></inline-formula> and <inline-formula> <tex-math notation="LaTeX">11.16\times 10^{{10}}~\text {cm}\cdot \text {Hz}^{{0.5}}\cdot \text {W}^{-{1}} </tex-math></inline-formula>, respectively. An analytic model was developed to discuss current amplification for different wavelengths when considering absorption efficiency and carrier transportation. The emitter thickness was optimized as 60 nm to significantly improve the current amplification under short wavelengths. The achieved optical responsivity of the optimized SiGe/Si HPT for 405 and 650 nm respectively were 13.756 and 13.904 A/W, and the specific detectivity were <inline-formula> <tex-math notation="LaTeX">12.41\times 10^{{10}} </tex-math></inline-formula> and <inline-formula> <tex-math notation="LaTeX">12.54\times 10^{{10}}~\text {cm}\cdot \text {Hz}^{{0.5}} \cdot \text {W}^{-{1}} </tex-math></inline-formula>.]]></abstract><pub>IEEE</pub><doi>10.1109/TED.2024.3467218</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0001-7914-9411</orcidid><orcidid>https://orcid.org/0000-0002-7534-1470</orcidid><orcidid>https://orcid.org/0000-0001-9775-5124</orcidid></addata></record>
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subjects Absorption
Dark current
Light detection
Noise
Optical device fabrication
Optical sensors
Photoconductivity
responsivity
Sensitivity
SiGe/Si heterojunction phototransistors (HPTs)
Silicon germanium
specific detectivity
Turning
Voltage measurement
title A SiGe/Si Heterojunction Phototransistor for High Sensitivity Light Detection
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