A Photon Counting Lidar Based on True Random Coding
A technology of photon counting and laser radar, which is applied to the re-radiation of electromagnetic waves, instruments, and measuring devices, can solve problems such as difficult engineering applications, low practicability, and poor ranging performance, so as to reduce measurement time and improve correlation , Improve the effect of ranging ability
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specific Embodiment approach 1
[0019] Specific implementation mode 1: see figure 1 This embodiment will be described. The photon counting lidar with true random encoding described in this embodiment includes a first Geiger mode avalanche photodiode 1, a pulse shaping circuit 2, a laser 3, an optical system 4, a second Geiger mode Mode avalanche photodiode 5, external clock 6, photon counting module 7 and signal processing module 8; the first Geiger mode avalanche photodiode 1 responds to thermal noise or background light noise, and its output is connected to the pulse shaping circuit. The input terminals are connected, and the pulse shaping circuit 2 shapes the electrical pulses to obtain a random sequence of narrow pulses. One of its output terminals is connected to the first channel of the photon counting module 7 to obtain the reference template a(n) of the random sequence, and the other The output end is connected to the input end of the laser 3. The laser 3 receives the electrical pulses from the pulse...
specific Embodiment approach 2
[0020] Embodiment 2: The difference between this embodiment and the photon-counting lidar with random encoding described in Embodiment 1 is that the specific process of generating a real machine code sequence is as follows:
[0021] When the first Geiger mode avalanche photodiode 1 is powered on, due to the thermal noise of the detector itself, even in the dark room, there will be pulses, which are called dark counts, and the number of dark counts is the same as that of the first Geiger mode avalanche. The operating temperature of the photodiode is related. At the same time, the first Geiger mode avalanche photodiode 1 also responds to the incident background light. Through the response to dark noise and background light noise, the final periodic output pulse random sequence. The periodic output of the pulse sequence is mainly realized by adding a gate control circuit to the first Geiger mode avalanche photodiode 1. The first Geiger mode avalanche photodiode 1 is in an enable...
specific Embodiment approach 3
[0022] Embodiment 3: The difference between this embodiment and the photon counting lidar with true random encoding described in Embodiment 2 is that the photon counting lidar system with true random encoding described in Embodiment 3 implements specific ranging. The process is:
[0023] The laser 3 receives the electrical pulse sequence generated from the second embodiment, modulates the continuous laser light into a random optical pulse sequence according to the input random electrical pulse sequence, and the output optical pulse sequence is irradiated to the target through the optical system 4, and is scattered by the target. A part of the laser echo signal will be returned to the optical system 4, and sent to the second Geiger mode avalanche photodiode 5 through the optical system 4, and the second Geiger mode avalanche photodiode 5 will output electrical pulses in response to the laser echo signal, and The electrical pulse signal of the second Geiger mode avalanche photod...
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