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Schematic of a system based on DTDM: FPGA, field programmable gate array; TL, transmitting lens; RL, receiving lens; APD, Avalanche photo diode; TD, time delayer; and SSM, signal sampling module.

Schematic of a system based on DTDM: FPGA, field programmable gate array; TL, transmitting lens; RL, receiving lens; APD, Avalanche photo diode; TD, time delayer; and SSM, signal sampling module.

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A ranging method based on the differential time domain method (DTDM) is proposed in order to improve ranging accuracy and the range of active measurement based on peak discriminator (PD). We develop mathematical models and deduce that zero-crossing sensitivity is an important factor, which affects the ranging error of DTDM. Additionally, zero-cross...

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... In D-ToF LiDAR systems, semiconductor photodetectors are commonly employed due to their small size, low cost, and insensitivity to magnetic fields. Among these, linear and Geigermode avalanche photodiodes (APDs) are the most commonly used types [5][6][7][8]. ...
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... The main ranging methods can be divided into time identification methods based on the time-to-digital converter (TDC) and waveform centroid determination. When the environment and the target are more complex, the amplitude of the echo pulse changes greatly, and the TDC technology that only relies on the threshold to achieve time measurement will no longer be suitable, leading to a large drift error [5][6][7][8]. The full waveform ranging method is the most effective method to solve this problem, mainly including the waveform centroid and Gaussian fitting methods. ...
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We theoretically and experimentally examined the effects of the different positions between receiving lens (RL) and detector, namely, defocus, off-axis, and tilt, on the time-domain pulsed echo laser profile (TDPELP). Results show that distortions including saturation and broadening of TDPELP are obtained, regardless of the position between RL and detector. Thus, we adjust the focal length of RL to successfully obtain an optimal TDPELP using tunable lens under extreme situations, such as too strong or too weak intensity of the TDPELP.