<p>In this work, we present a novel avalanche photodiode (APD) that utilizes the <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11885_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{Si}}_{1-\text{x}}{\text{Sn}}_{\text{x}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Si</mtext> <mrow> <mn>1</mn> <mo>-</mo> <mtext>x</mtext> </mrow> </msub> <msub> <mtext>Sn</mtext> <mtext>x</mtext> </msub> </mrow> </math></EquationSource> </InlineEquation>-on-silicon (SiSn-on-Si) platform to enable short-wave infrared (SWIR) operation. This work reports the first proof of the <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11885_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{Si}}_{1-\text{x}}{\text{Sn}}_{\text{x}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Si</mtext> <mrow> <mn>1</mn> <mo>-</mo> <mtext>x</mtext> </mrow> </msub> <msub> <mtext>Sn</mtext> <mtext>x</mtext> </msub> </mrow> </math></EquationSource> </InlineEquation> alloy-based APD. Here, we propose two device structures—<i>p</i><sup><i>+</i></sup><i>-i-p-i-n</i><sup><i>+</i></sup> (device D1) and <i>n</i><sup><i>+</i></sup><i>-i-n-i-p</i><sup><i>+</i></sup> (device D2)—and we use COMSOL Multiphysics to analyze their performance. With the insertion of Sn into the <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11885_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{Si}}_{1-\text{x}}{\text{Sn}}_{\text{x}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Si</mtext> <mrow> <mn>1</mn> <mo>-</mo> <mtext>x</mtext> </mrow> </msub> <msub> <mtext>Sn</mtext> <mtext>x</mtext> </msub> </mrow> </math></EquationSource> </InlineEquation> alloy, the bandgap energy decreases, and the detection wavelength is redshifted toward a longer wavelength. As a result, this work presents the breakthrough of Si-based detectors, demonstrating significant advancements in the field. Moreover, the high absorption coefficient of the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11664_2025_11885_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{Si}}_{1-\text{x}}{\text{Sn}}_{\text{x}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Si</mtext> <mrow> <mn>1</mn> <mo>-</mo> <mtext>x</mtext> </mrow> </msub> <msub> <mtext>Sn</mtext> <mtext>x</mtext> </msub> </mrow> </math></EquationSource> </InlineEquation> alloy over pure Si results in high responsivity. The separate absorption, charge, and multiplication (SACM) device structure allows for a substantial performance improvement, with device D1 achieving a high multiplication gain of over 77 and device D2 achieving a multiplication gain of over 80 at a wavelength of 1310 nm and a temperature of 300 K. Our proposed SiSn-on-Si APD shows a significant reduction in excess noise factor compared to the In<sub>0.52</sub>Al<sub>0.48</sub>As device. In addition, when compared to previously reported Si/Ge APDs, the SiSn-on-Si APD demonstrates superior performance in terms of gain, responsivity, and the low bias voltage required for operation. These findings, using the cost-effective SiSn-on-Si platform, provide a pathway for the future development of high-performance Si-based APDs for use in the SWIR bands.</p>

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High-Performance Si1−xSnx/Si Avalanche Photodiode on Si Platform at Room Temperature

  • Harshvardhan Kumar,
  • Advaita Sinha,
  • Chushou Yang

摘要

In this work, we present a novel avalanche photodiode (APD) that utilizes the \({\text{Si}}_{1-\text{x}}{\text{Sn}}_{\text{x}}\) Si 1 - x Sn x -on-silicon (SiSn-on-Si) platform to enable short-wave infrared (SWIR) operation. This work reports the first proof of the \({\text{Si}}_{1-\text{x}}{\text{Sn}}_{\text{x}}\) Si 1 - x Sn x alloy-based APD. Here, we propose two device structures—p+-i-p-i-n+ (device D1) and n+-i-n-i-p+ (device D2)—and we use COMSOL Multiphysics to analyze their performance. With the insertion of Sn into the \({\text{Si}}_{1-\text{x}}{\text{Sn}}_{\text{x}}\) Si 1 - x Sn x alloy, the bandgap energy decreases, and the detection wavelength is redshifted toward a longer wavelength. As a result, this work presents the breakthrough of Si-based detectors, demonstrating significant advancements in the field. Moreover, the high absorption coefficient of the \({\text{Si}}_{1-\text{x}}{\text{Sn}}_{\text{x}}\) Si 1 - x Sn x alloy over pure Si results in high responsivity. The separate absorption, charge, and multiplication (SACM) device structure allows for a substantial performance improvement, with device D1 achieving a high multiplication gain of over 77 and device D2 achieving a multiplication gain of over 80 at a wavelength of 1310 nm and a temperature of 300 K. Our proposed SiSn-on-Si APD shows a significant reduction in excess noise factor compared to the In0.52Al0.48As device. In addition, when compared to previously reported Si/Ge APDs, the SiSn-on-Si APD demonstrates superior performance in terms of gain, responsivity, and the low bias voltage required for operation. These findings, using the cost-effective SiSn-on-Si platform, provide a pathway for the future development of high-performance Si-based APDs for use in the SWIR bands.