FIELD: optical technology.
SUBSTANCE: invention relates to the reception of optical signals, in particular to the technique of receiving signals using avalanche photodiodes, and can be used in location, communication and other photoelectronic systems. The method for threshold detection of optical signals using an avalanche photodiode includes threshold signal processing and the formation of output pulses using a threshold device when the signal from the output of the photodiode exceeds the specified trigger threshold. In this case, the non-multipliable component of the square of the noise current brought to the output of the photodiode is preliminarily determined, and the second threshold Ithr2, brought to the output of the photodiode, is set within the limits of , the square of the non-multipliable noise current brought to the output of the photodiode. The bias voltage of the photodiode is set at a level at which the signal-to-noise ratio is maximum, after which the offset voltage is reduced until the estimate ϕ2 of the relative frequency of exceeding the threshold Ithr2 by microplasma emissions drops to the maximum permissible level where is the number of allowed intervals at the control interval T2; ΔT is the allowed time interval; n2 the number of exceedances of the threshold Ithr2 during T2; QM is the permissible probability of occurrence of microplasmas during T2; t is the parameter of the statistical spread of the estimate ϕ2. After that, the bias voltage is fixed and the threshold Ithr1 is set at a level at which the frequency f1 (1/s) of noise exceeding the threshold Ithr1 has a stationary value f1 << f0, where f0 is the frequency of noise crossing the zero level. At the same time, the input of Ithr1 is blocked for the time of each exceeding of the threshold of Ithr2. After setting the threshold Ithr1, it is increased by a factor of , where fp is the maximum permissible frequency of false alarms in operating mode. Then the threshold Ithr1 is fixed and signals are received.
EFFECT: achieving the maximum sensitivity in all operating conditions, taking into account microplasma breakdowns and normal noise with a minimum time to reach the optimal avalanche mode.
2 cl, 2 dwg
Title | Year | Author | Number |
---|---|---|---|
METHOD FOR RECEIVING PULSED OPTICAL SIGNALS | 2021 |
|
RU2778048C1 |
LASER PULSE RANGEFINDER | 2022 |
|
RU2791186C1 |
METHOD FOR INCOHERENT ACCUMULATION OF PULSED LIGHT-LOCATION SIGNALS | 2022 |
|
RU2791151C1 |
METHOD FOR STABILIZING THE AVALANCHE PHOTODIODE MODE | 2021 |
|
RU2778976C1 |
METHOD FOR STABILIZING THE AVALANCHE MODE OF A PHOTODIODE | 2021 |
|
RU2778045C1 |
METHOD FOR RECEIVING OPTICAL SIGNALS | 2021 |
|
RU2778047C1 |
METHOD FOR PULSE LOCATION RANGING | 2022 |
|
RU2792086C1 |
METHOD FOR INCOHERENT ACCUMULATION OF LIGHT-LOCATION SIGNALS | 2022 |
|
RU2788940C1 |
METHOD FOR RECEIVING OPTICAL PULSES | 2021 |
|
RU2778046C1 |
METHOD FOR DETECTING OPTICAL SIGNALS | 2020 |
|
RU2755601C1 |
Authors
Dates
2022-08-22—Published
2021-11-22—Filed