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Compared to detection methods such as cameras and millimeter-wave radar, LiDAR (light detection and ranging) utilizes a highly collimated laser beam to obtain target distance, azimuth, shape, and motion information, providing superior three-dimensional perception capabilities. In the early days, LiDAR was primarily used in military, surveying, environmental monitoring, and other fields, given its large size and high cost. However, LiDAR has gradually integrated into the consumer market and played an increasingly crucial role in autonomous driving and intelligent perception, becoming a hot research topic in recent years. The primary functions of LiDAR can be divided into scanning imaging modules. As weight, size, and power consumption become crucial for platforms such as automobiles and drones, traditional mechanical LiDAR systems are evolving toward solid-state scanning approaches. Among various scanning devices, MEMS (micro-electro-mechanical systems) mirrors have become a hot direction in LiDAR scanning due to their small size, low power consumption, and high angular resolution. With the advancement of LiDAR technology, the scanning field of view of MEMS devices continues to increase, resulting in increasingly stringent requirements for matching the emission and reception fields of view.
The influence of MEMS deflection angle on the received power was derived based on the laser radar equation in this study. Detailed design specifications for the lidar system were analyzed, along with the achievable detection distance range. A suitable receiving scheme for MEMS-based short-range laser radar was proposed, where a single-piece non-spherical mirror was used for beam collimation at the transmitting end, and a small sensitive area InGaAs detector operating at 1550 nm was employed at the receiving end to address the problem of inefficient echo reception for larger scanning fields of the MEMS system. A receiver device suitable for near-range wide field-of-view applications has been designed. The optical system at the receiving end utilizes an afocal telecentric structure as the receiving antenna, achieving a reception field-of-view of 36° at a photosensitive area of 1 mm. The relative illuminance exceeds 95%, demonstrating excellent light collection and transmission characteristics. Additionally, the receiver circuit adopts a T-network amplification structure combined with a moment identification circuit, utilizing the TDC7200 to achieve high-precision time measurements. The flight time measurement accuracy is less than 120 ps within a range of 200 ns, and the overall experimental results demonstrate ranging accuracy better than 2 ns within an 8 m distance, meeting the requirements for near-range detection.
System overall structure diagram
MEMS scanning spot array with varying diameters. (a) Spot diameter of 3 mm; (b) Spot diameter of 5 mm
Variation of light spot diameter with different focal lengths
Angular distribution of MEMS light spot deviations
MEMS deflection angle and echo power correlation
Optical antenna structure for reception
Surface track image of the detector
Geometric ring entrance energy map
Distribution of relative illuminance in different fields of view
Wide angle echo reception circuit
Design of TDC7200 time measurement
TDC7200 internal working mechanism
TDC time measurement process flowchart
Histogram of actual measurement with 150 ns
Measurement error of TDC in actual conditions
Receiving physical devices
Time distribution of testing at a distance of 6 m
Actual indoor scene testing
100 kHz echo waveform