THIRD-HARMONIC GENERATING APPARATUS FOR LASER-RADIATION

• US 20200132906A1
• Filed: 10/26/2018
• Published: 04/30/2020
• Est. Priority Date: 10/26/2018
• Status: Active Grant

• Current Assignee: Coherent Inc (Coherent Corp.)
• Original Assignee: Coherent Inc (Coherent Corp.)
• Inventors: CAPRARA, Andrea
• Granted Patent: US 10,983,260 B2
• Time in Patent Office: Days
• CPC Class Codes: G02B 27/0977 Reflective elements
• CPC Class Codes: G02B 5/08 Mirrors vehicle mirrors involving special optical features B60R1/08
• CPC Class Codes: G02B 5/3025 Polarisers, i.e. arrangements capable of producing a definite output polarisation state from an unpolarised input state G02B5/3008, G02B5/3016 take precedence
• CPC Class Codes: G02F 1/3532 Arrangements of plural nonlinear devices for generating multi-colour light beams, e.g. arrangements of SHG, SFG, OPO devices for generating RGB light beams
• CPC Class Codes: G02F 1/3534 Three-wave interaction, e.g. sum-difference frequency generation G02F1/3532 takes precedence
• CPC Class Codes: G02F 1/354 Third or higher harmonic generation
• CPC Class Codes: H01S 3/0085 Modulating the output, i.e. the laser beam is modulated outside the laser cavity

Abstract

A third-harmonic conversion arrangement includes a second-harmonic generating crystal and a third-harmonic generating crystal arranged in a polarization loop. The polarization loop causes plane-polarized fundamental-wavelength radiation being converted to make two passes through the crystals in orthogonally-opposed polarization orientations.

Claims

1. Optical apparatus for generating third-harmonic radiation from plane-polarized fundamental radiation, comprising:

a polarization loop including a plurality of mirrors, a polarization-selective reflector and a polarization rotator, the polarization loop arranged such that the fundamental radiation enters the loop via the polarization-selective reflector, makes a first circuit of the loop, makes a second circuit of the loop, and then exits the loop via the polarization-selective reflector, at each location on the loop the fundamental radiation on the first circuit of the loop having a polarization orientation orthogonal to the polarization orientation of the fundamental radiation on the second circuit of the loop, the polarization rotator rotating the polarization of the fundamental radiation between the orthogonal polarization orientations; and

first and second optically nonlinear crystals located in the polarization loop, the first optically nonlinear crystal arranged to generate second-harmonic radiation by frequency doubling fundamental radiation on the second circuit of the loop, and the second optically nonlinear crystal arranged to generate the third-harmonic radiation by sum-frequency mixing second-harmonic radiation generated in the first optically nonlinear crystal and fundamental radiation on the first circuit of the loop.

2. The apparatus of claim 1, wherein the frequency doubling is type-1 and the sum-frequency mixing is type 1.

3. The apparatus of claim 1, wherein the full power of the fundamental radiation is available for the third-harmonic generation and fundamental radiation depleted by the third-harmonic generation is used to generate the second-harmonic radiation.

4. The apparatus of claim 1, wherein the plurality of mirrors includes first, second and third mirrors numbered in consecutive numerical order from the polarization-selective reflector in the direction of circulation of the fundamental radiation, and wherein the first and second optically nonlinear crystals are located between the polarization-selective reflector and the first mirror, the first optically nonlinear crystal being closest to the polarization-selective reflector.

5. The apparatus of claim 4, wherein the first mirror is a dichroic reflector arranged to reflect the fundamental radiation and transmit the second-harmonic radiation and the third-harmonic radiation.

6. The apparatus of claim 1, wherein the fundamental radiation is near-infrared radiation.

7. The apparatus of claim 1, wherein the fundamental radiation has a wavelength of 1064 nanometers, the second-harmonic radiation has a wavelength of 532 nanometers, and the third-harmonic radiation has a wavelength of 355 nanometers.

8. The apparatus of claim 1, wherein the fundamental radiation is a pulse.

9. The apparatus of claim 8, wherein the pulse has a duration of greater than three times a round-trip time of the polarization loop.

10. The apparatus of claim 8, wherein the pulse has a duration of less than about 50 picoseconds.

11. The apparatus of claim 1, wherein the fundamental radiation is a beam of ultrashort pulses, a round-trip time of the loop being synchronous with a pulse repetition rate of the ultra short pulses.

12. Optical apparatus for generating third-harmonic radiation from plane-polarized fundamental radiation, comprising:

a polarization loop including a plurality of mirrors, a polarization-selective reflector and a polarization rotator, the polarization loop arranged such that the fundamental radiation enters the loop via the polarization-selective reflector, makes a first circuit of the loop, makes a second circuit of the loop, and then exits the loop via the polarization-selective reflector, the fundamental radiation plane-polarized in a first orientation on the first circuit of the loop between the polarization-selective reflector and the polarization rotator, the fundamental radiation polarized in a second orientation orthogonal to the first orientation on the second circuit of the loop between the polarization-selective reflector and the polarization rotator, the polarization rotator rotating the polarization of the fundamental radiation between the first orientation and the second orientation; and

first and second optically nonlinear crystals located in the polarization loop between the polarization-selective reflector and the polarization rotator, the first optically nonlinear crystal arranged to generate second-harmonic radiation by frequency doubling fundamental radiation on the second circuit of the loop, and the second optically nonlinear crystal arranged to generate the third-harmonic radiation by sum-frequency mixing second-harmonic radiation generated in the first optically nonlinear crystal and fundamental-wavelength radiation on the first circuit of the loop.

13. The apparatus of claim 12, wherein the frequency doubling is type-1 and the sum-frequency mixing is type 1.

14. The apparatus of claim 12, wherein the full power of the fundamental radiation is available for the third-harmonic generation and fundamental radiation depleted by the third-harmonic generation is used to generate the second-harmonic radiation.

15. The apparatus of claim 12, wherein the plurality of mirrors includes first, second and third mirrors numbered in consecutive numerical order from the polarization-selective reflector in the direction of circulation of the fundamental radiation, and wherein the first and second optically nonlinear crystals are located between the polarization-selective reflector and the first mirror, the first optically nonlinear crystal being closest to the polarization-selective reflector.

16. The apparatus of claim 12, wherein the fundamental radiation is a pulse.

17. The apparatus of claim 16, wherein the pulse has a duration of greater than three times a round-trip time of the polarization loop.

18. The apparatus of claim 16, wherein the pulse has a duration of less than about 50 picoseconds.

19. The apparatus of claim 12, wherein the fundamental radiation is a beam of ultrashort pulses, a round-trip time of the loop being synchronous with a pulse repetition rate of the ultrashort pulses.