IP Library Granted Patent US 11,835,656
Granted Patent B2
US 11,835,656 · App. 17/142,616 · Granted Dec 5, 2023

Methods for scanning a LiDAR system in two dimensions

Inventors: Jun Pei (Saratoga, CA); Mark A. McCord (Los Gatos, CA); Roger David Cullumber (Hollister, CA); Yupeng Cui (San Jose, CA); Dongyi Liao (Mountain View, CA)
Assignee: Cepton Technologies, Inc.
G01S7/4817G01S7/4815G01S17/42G01S17/89
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Quick Facts
Patent No.
US 11,835,656
App. No.
17/142,616
Granted
Dec 5, 2023
Kind
B2
Abstract

A method of three-dimensional imaging includes scanning a LiDAR system in a first direction with a first frequency and in a second direction with a second frequency that is different from the first frequency, so that a laser beam emitted by each laser source of the LiDAR system follows a Lissajous pattern. The method further includes emitting, using each laser source, a plurality of laser pulses as the LiDAR system is scanned in the first direction and the second direction; detecting, using each detector of the LiDAR system, a portion of each laser pulse of the plurality of laser pulses reflected off of one or more objects; determining, using a processor, a time of flight for each respective laser pulse from emission to detection; and acquiring a point cloud of the one or more objects based on the times of flight of the plurality of laser pulses.

Claims (16)

1. A method of three-dimensional imaging using a LiDAR system, the method comprising:

scanning the LiDAR system in a first direction with a first frequency and in a second direction orthogonal to the first direction with a second frequency, the LiDAR system including an electro-optic assembly that comprises one or more laser sources and one or more detectors, each respective detector corresponding a respective laser source, wherein the scanning of the LiDAR system in the first direction and the second directions scans a laser beam emitted by each respective laser source across a respective sub-field of view, and wherein the second frequency differs from the first frequency such that a trajectory of each laser source follows a Lissajous pattern;

translating the electro-optic assembly in the first direction and the second direction in a plane that is substantially perpendicular to an optical axis of the LiDAR system;

emitting, using each of the one or more laser sources, a plurality of laser pulses as the LiDAR system is scanned in the first direction and the second direction;

detecting, using each of the one or more detectors, a portion of each respective laser pulse of the plurality of laser pulses reflected off of one or more objects;

determining, using a processor, a time of flight for each respective laser pulse from emission to detection; and

acquiring a point cloud of the one or more objects based on the times of flight of the plurality of laser pulses from each laser source.

2. The method of claim 1 further comprising outputting the point cloud at a frame rate that is equal to a difference between the second frequency and the first frequency, so that that the trajectory of each laser source completes a full Lissajous scan pattern in each frame.

3. The method of claim 1 further comprising outputting the point cloud at a frame rate that is equal to one half of a difference between the second frequency and the first frequency, so that that the trajectory of each laser source completes two full Lissajous scan patterns in each frame.

4. The method of claim 1 further comprising outputting the point cloud at a frame rate that is equal to a fraction of a difference between the second frequency and the first frequency, so that that the trajectory of each laser source completes an integer number of full Lissajous scan patterns in each frame, wherein the integer number is greater than two.

5. The method of claim 1 wherein:

the electro-optic assembly is flexibly coupled to a fixed frame via a flexure assembly; and

translating the electro-optic assembly is performed via the flexure assembly.

6. The method of claim 5 wherein:

the flexure assembly has a first resonant frequency in the first direction, and a second resonant frequency in the second direction; and

the first frequency is substantially equal to the first resonant frequency, and the second frequency is substantially equal to the second resonant frequency.

Assignments (3)
RELEASE OF SECURITY INTEREST Recorded Jan 25, 2023
From: KOITO MANUFACTURING CO., LTD.
To: CEPTON TECHNOLOGIES, INC., A DELAWARE CORPORATION
Reel/Frame 062485/0955 →
SECURITY INTEREST Recorded Nov 8, 2022
From: CEPTON TECHNOLOGIES, INC.
To: KOITO MANUFACTURING CO., LTD.
Reel/Frame 061690/0653 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 6, 2021
From: PEI, JUN; MCCORD, MARK A.; CULLUMBER, ROGER DAVID; CUI, YUPENG; LIAO, DONGYI
To: CEPTON TECHNOLOGIES, INC.
Reel/Frame 054829/0577 →
Continuity (3)
Division 15971548 · May 4, 2018
Provisional Application 62574549 · Oct 19, 2017
Related Publication 20210141065A1 · May 13, 2021
Cited By (1)
US 12,468,043