Photonics Research, Volume. 10, Issue 8, 1956(2022)

Three-terminal germanium-on-silicon avalanche photodiode with extended p-charge layer for dark current reduction

Xiaobin Liu1, Xuetong Li1, Yuxuan Li1, Yingzhi Li1, Zihao Zhi1, Min Tao1, Baisong Chen1, Lanxuan Zhang1, Pengfei Guo2, Guoqiang Lo2, Xueyan Li1, Fengli Gao1, Bonan Kang1, and Junfeng Song1,3、*
Author Affiliations
  • 1State Key Laboratory of Integrated Optoelectronics, College of Electronic Science and Engineering, Jilin University, Changchun 130012, China
  • 2Advance Micro Foundry Pte Ltd, Singapore 117685, Singapore
  • 3Peng Cheng Laboratory, Shenzhen 518000, China
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    Figures & Tables(15)
    (a) Structural diagram of three-terminal Ge-on-Si APD. (b) SEM image of pixel units. (c) Electric field simulation diagram of Ge region. (d) Simulated electric field in Si APD area [electric field at different positions of line A in (b)].
    (a) Current characteristic diagram at 1550 nm under different input optical power. (b) Responsivity characteristic diagram at 1550 nm under different input optical power. (c) Current characteristic diagram at 1310 nm under different input optical power. (d) Responsivity characteristic diagram at 1310 nm under different input optical power. The figure shows the voltage applied to two terminals Ge and n++ Si.
    It represents the simulated dark current diagram (current output at the n++ terminal) when different fixed voltages are applied to Ge when the n++ Si voltage is 60 V and p++ Si is grounded.
    When the n++ Si terminal scanning voltage is 60 V, the p++ Si terminal is grounding, and different fixed voltages are applied to Ge: (a) dark current; (b) current characteristic diagram at 1550 nm under input optical power −20 dBm. (c) Under the fixed Si voltage, the dark current of n++ Si terminal varies with the applied voltage of Ge. (d) Under the fixed Si voltage, the current at 1550 nm at an input optical power of −20 dBm varies with the applied voltage of Ge.
    (a) Schematic diagram of three-terminal APD. (b) Y direction electric field simulation in Si region [position from B to B′ in (a)]. (c) X direction electric field simulation of Si charge region [position from A to A′ in (a)]. (d) Electric field simulation diagram of Ge region.
    (a) Photocurrent diagram at 10−7 A. (b) Responsivity at 10−7 A. (c) Photocurrent diagram at 10−8 A. (d) Responsivity at 10−8 A.
    When the voltage on Ge is −27.5 V. (a) Current characteristic diagram at 1310 nm under different input optical power. (b) Responsivity characteristic diagram at 1310 nm under different input optical power. (c) Current characteristic diagram at 1550 nm under different input optical power. (d) Responsivity characteristic diagram at 1550 nm under different input optical power.
    When the voltage on Ge is −27.5 V. (a) Avalanche gain at 1310 nm wavelength. (b) Avalanche gain at 1550 nm wavelength.
    When the applied voltage on p++ Ge is −27.5 V and the input optical power is −20 dBm. (a) Responsivity in O-band. (b) Responsivity in C-band (1530–1560 nm) and L-band (1570–1600 nm).
    (a) Current at −20 V on Ge. (b) Current at −25 V on Ge. (c) Current at −30 V on Ge. (d) At different voltages on Ge, the photocurrent is greater than the multiple of dark current.
    (a) The APD has a normalized RF response characteristic at a voltage of Ge at −27.5 V and different Si input voltages. (b) The APD voltage on the Ge is −27.5 V, and the S22 parameters are measured under different Si input voltages. (c) The APD has a normalized RF response characteristic at a voltage of Si at 15 V and different Ge input voltages. (d) The APD voltage on the Si is 15 V, and the S22 parameters are measured under different Ge input voltages [the specific voltage values are shown in (c)].
    (a) When the voltage is −27.5 V on Ge, the three-terminal APD equivalent circuit model. (b) When the signal ends are input to 15 V, the reflection coefficient is measured and fitted. (c) The relative error values between simulation and practice in (b).
    • Table 1. Response of Ge to −27.5 V at Different Input Power

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      Table 1. Response of Ge to −27.5 V at Different Input Power

       10  dBm20  dBm30  dBm40  dBm
      R1 at 1310 nm0.80 A/W3.16 A/W6.17 A/W10.50 A/W
      R2 at 1310 nm0.63 A/W1.80 A/W1.82 A/W1.74 A/W
      R1 at 1550 nm0.83 A/W3.55 A/W6.96 A/W9.97 A/W
      R2 at 1550 nm0.68 A/W2.36 A/W2.48 A/W2.07 A/W
    • Table 2. Fitted Electric Circuit Parameters of a Three-Terminal Avalanche Photodiode under a Reverse Bias of 15 V

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      Table 2. Fitted Electric Circuit Parameters of a Three-Terminal Avalanche Photodiode under a Reverse Bias of 15 V

      ParametersLp (nH)Rs(kΩ)Cd (fF)Rd(kΩ)
      Values13751.21452.41
      ParametersCc(pF)Lm(μH)Rm  (kΩ)Cm(pF)
      Values2.819.80.8254.2
      ParametersLa(μH)Ra(kΩ)Ca(fF)
      Values1961172
    • Table 3. Device Performance of Surface Illuminated APDs

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      Table 3. Device Performance of Surface Illuminated APDs

      Referenceλ (nm)Dark Current (A)Responsivity (A/W)
      [34]13108.4×1076.54
      [10]131010512.00
      [35]155010412.70
      [36]13101064.40
      [33]13101065.88
      This work131010710.50
      This work15501079.97
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    Xiaobin Liu, Xuetong Li, Yuxuan Li, Yingzhi Li, Zihao Zhi, Min Tao, Baisong Chen, Lanxuan Zhang, Pengfei Guo, Guoqiang Lo, Xueyan Li, Fengli Gao, Bonan Kang, Junfeng Song, "Three-terminal germanium-on-silicon avalanche photodiode with extended p-charge layer for dark current reduction," Photonics Res. 10, 1956 (2022)

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    Paper Information

    Category: Silicon Photonics

    Received: Dec. 22, 2021

    Accepted: Jun. 13, 2022

    Published Online: Jul. 27, 2022

    The Author Email: Junfeng Song (songjf@jlu.edu.cn)

    DOI:10.1364/PRJ.452004

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