Journal of Infrared and Millimeter Waves, Volume. 44, Issue 3, 327(2025)

Research on the punch-through phenomenon of separate absorption, charge and multiplication avalanche photodetectors

Chong LI1、*, Zi-Yi MA1, Shuai YANG1, Yue-Wen LIU1, Jia-Xuan WANG1, Yun-Fei LIU2, Yu-Sen DONG1, Zi-Qian LI1, and Dian-Bo LIU1
Author Affiliations
  • 1Key Laboratory of Optoelectronics Technology of Ministry of Education, School of Information Science and Technology, Beijing University of Technology, Beijing 100124, China
  • 2Institute of Advanced Semiconductor Optoelectronic Technology, School of Physics and Optoelectronic Engineering, Beijing University of Technology, Beijing 100124, China
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    Figures & Tables(7)
    Schematic diagram of device structure: (a) schematic of cross-section of the fabricated SACM APD; (b) SEM image
    Schematic diagram of device structure simulation: (a) internal electric field of the device at different reverse biases,The inset shows the feedback electric field at the interface between electric field control layer and absorption layer; (b) simulated I-V characteristics and multiplication factor of the SACM APD; (c) energy band diagrams before punch-through; (d) energy band diagrams after punch-through; (e) doping concentration diagram of the device, when the ion implantation energy is 580 keV
    I-V characteristics of SACM APD and dark current characteristics of SACM APD with different sizes: (a) I-V characteristics and multiplication factor of 100 μm SACM APD; (b) the dark current curves of devices with photosensitive surface radii of 20 μm, 50 μm, 100 μm and 200 μm; (c) relationships between the dark current and the photosensitive area radius at -30 V, the red line is the fitting curve according to Eq. (1)
    I-V characteristics and spectral response of SACM APD: (a) I-V characteristics of 100 μm SACM APD with different input light wavelengths; (b) spectral response of 100 μm SACM APD at different reverse biases
    C-V characteristics of SACM APD:(a) C-V characteristics of 100μm SACM APD at 100 kHz,200 kHz,500 kHz,1 MHz and 5 MHz, respectively; (b) C-V characteristics of devices with different photosensitive surface radii at 1 MHz (dashed line represents the simulation result for devices with a radius of 100 μm at 1 MHz) ;(c) fitting relationships between the capacitance value and the device photosensitive area at 0 V, -20 V and -30 V bias
    Temperature characteristics of SACM APD: (a) dark current of 200 μm SACM APD versus voltage at different temperatures; (b) the relationship between dark current and temperature at -20 V and -30 V bias
    • Table 1. Comparison of photocurrent and absorption coefficient before and after punch-through under different wavelengths of input light

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      Table 1. Comparison of photocurrent and absorption coefficient before and after punch-through under different wavelengths of input light

      Wavelength

      λ/nm

      Photocurrent before punch-through

      Ibefore /μA

      Photocurrent after punch-through

      Iafter /μA

      Iafter/Ibefore

      Absorption coefficient

      α /cm-1

      4050.790.861.0895 000
      5050.631.041.6511 000
      63521.8341.871.923 200
      8086.3113.772.18775
      850134.83212.771.58535
      1 0640.100.181.8011
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    Chong LI, Zi-Yi MA, Shuai YANG, Yue-Wen LIU, Jia-Xuan WANG, Yun-Fei LIU, Yu-Sen DONG, Zi-Qian LI, Dian-Bo LIU. Research on the punch-through phenomenon of separate absorption, charge and multiplication avalanche photodetectors[J]. Journal of Infrared and Millimeter Waves, 2025, 44(3): 327

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    Paper Information

    Category: Infrared Physics, Materials and Devices

    Received: Sep. 10, 2024

    Accepted: --

    Published Online: Jul. 9, 2025

    The Author Email: Chong LI (lichong@bjut.edu.cn)

    DOI:10.11972/j.issn.1001-9014.2025.03.001

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