Light detection and ranging (LiDAR) system using a wavelength converter

1. A system for detecting laser light returned from an object, comprising:

a transmitter comprising:

one or more laser sources, at least one of the laser sources configured to provide a respective native laser beam having a wavelength above 1,100 nm;

a wavelength converter configured to receive the native laser beams provided by the laser sources and convert the native laser beams into a converted laser beam having a wavelength below 1,100 nm; and

a scanner configured to emit the converted laser beam to the object in a first direction; and

a receiver configured to detect a returned laser beam having a wavelength below 1,100 nm and returned from the object in a second direction,

wherein when the laser sources include two laser sources providing two native laser beams, respectively, the wavelength of the converted laser beam is determined by

1

λ

3

=

1

λ

2

+

1

λ

1

where λ 3 represents the wavelength of the converted laser beam, and λ 1 and λ 2 each represents a respective wavelength of the two native laser beams.

2. The system of claim 1 , wherein at least one of the laser sources is a fiber laser.

3. The system of claim 2 , wherein each of the laser sources is a fiber laser.

4. The system of claim 3 , wherein the receiver includes a silicon-based photodetector.

5. The system of claim 3 , wherein the wavelength converter comprises:

a nonlinear optical material configured to perform optical frequency mixing of the native laser beams; and

a temperature controller configured to set a temperature of the nonlinear optical material based on the wavelength of the converted laser beam.

6. The system of claim 5 , wherein the nonlinear optical material includes a nonlinear optical crystal.

7. The system of claim 1 , wherein a number of the laser sources is not larger than 3.

8. The system of claim 7 , wherein when the laser sources include three laser sources providing three native laser beams, respectively, the wavelength of the converted laser beam is determined by

1

λ

4

=

1

λ

3

+

1

λ

2

+

1

λ

1

where λ 4 represents the wavelength of the converted laser beam, and λ 1 , λ 2 , and λ 3 each represents a respective wavelength of the three native laser beams.

9. The system of claim 8 , wherein at least one of λ 1 , λ 2 , and λ 3 has a negative weight.

10. The system of claim 9 , wherein one of λ 1 , λ 2 , and λ 3 has a negative weight.

11. The system of claim 1 , wherein the laser sources include one laser source providing one native laser beam, and the wavelength of the converted laser beam is half of a wavelength of the native laser beam.

12. The system of claim 1 , wherein the laser sources include one laser source providing one native laser beam, and the wavelength of the converted laser beam is a third of a wavelength of the native laser beam.

13. An apparatus for emitting laser light, comprising:

a plurality of fiber lasers, each configured to provide a respective native laser beam having a first wavelength;

a wavelength converter configured to receive the native laser beams provided by the fiber lasers and convert the native laser beams into a converted laser beam having a second wavelength below the first wavelength; and

a scanner configured to emit the converted laser beam,

wherein the fiber lasers include three fiber lasers providing three native laser beams, respectively, and the wavelength of the converted laser beam is determined by

1

λ

4

=

1

λ

3

+

1

λ

2

+

1

λ

1

where λ 4 represents the wavelength of the converted laser beam, and λ 1 , λ 2 , and λ 3 each represents a respective wavelength of the three native laser beams.

14. The apparatus of claim 13 , wherein the wavelength converter comprises:

a nonlinear optical material configured to perform optical frequency mixing of the native laser beams; and

a temperature controller configured to set a temperature of the nonlinear optical material based on the wavelength of the converted laser beam.

15. The apparatus of claim 14 , wherein the nonlinear optical material includes a nonlinear optical crystal.

16. The apparatus of claim 13 , wherein the first wavelength is 1,100 nm.

17. A method for detecting laser light returned from an object, comprising:

providing, by a plurality of laser sources, a plurality of native laser beams, at least one of the laser beams having a wavelength above 1,100 nm;

converting, by a wavelength converter, the native laser beams into a converted laser beam having a wavelength below 1,100 nm;

emitting, by a scanner, the converted laser beam to the object in a first direction; and

detecting, by a receiver, a returned laser beam having a wavelength below 1,100 nm and returned from the object in a second direction,

wherein when the laser sources include two laser sources providing two native laser beams, respectively, the wavelength of the converted laser beam is determined by

1

λ

3

=

1

λ

2

+

1

λ

1

where λ 3 represents the wavelength of the converted laser beam, and λ 1 λ 2 each represents a respective wavelength of the two native laser beams.

18. The method of claim 17 , wherein converting the native laser beams into the converted laser beam comprises:

setting, by a temperature controller, a temperature of a nonlinear optical material based on the wavelength of the converted laser beam; and

performing, by the nonlinear optical material, optical frequency mixing of the native laser beams.