Equivalent circuit model establishing method of Ge/Si SACM structure avalanche photodiode
An equivalent circuit model, avalanche photoelectric technology, applied in electrical digital data processing, special data processing applications, instruments, etc., to achieve the effect of convenient simulation and design
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Embodiment 1
[0115] Under reverse bias, the incident light can be converted into output current, Figure 5 The simulation results of the I-V characteristics of the circuit model of Ge / Si SACM-APD are shown, where the dark current clearly shows the rectification behavior. At low bias voltage, the dark current is mainly affected by generation-recombination current and ohmic current. At high bias, additional dark current is induced by the tunneling current at the Ge / Si interface due to the avalanche multiplication effect of the APD. The avalanche breakdown voltage value of the circuit model designed by the present invention is 27.3V, so it can be seen that the simulation results can be consistent with the typical experimental results of 24V-28V.
Embodiment 2
[0117] Noise performance is an important index to identify the performance of photodetectors. Noise evaluation plays a very important role in the application of photodetectors and reducing the influence of noise on signals. Figure 6 The shot noise curves under different input optical power conditions are given. Such as Figure 6 As shown, the shot noise of the APD increases with the increase of the optical power, because the mean value of the square of the noise current of the APD is proportional to the size of the photogenerated current. But it is worth noting that the noise current curve changes relatively flat at low bias voltage, and it does not increase sharply with the increase of bias voltage until it is close to the breakdown voltage. This is due to the increase of reverse bias voltage. The increase in ionization coefficient and photocurrent.
Embodiment 3
[0119] The frequency response bandwidth reflects the high-speed performance of the photodetector in the frequency domain, Figure 7 The frequency response curves of the output under different reverse bias voltages are given. At low bias voltage, the bandwidth is mainly limited by the carrier transport time and RC constant, the lower frequency response increases with the increase of bias voltage, and decreases again when the bias voltage reaches -27V. However, at high bias, the bandwidth is mainly affected by the avalanche settling time, and the 3dB bandwidth decreases with increasing reverse bias. The above simulation results are in good agreement with the experimental results.
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