Controllable multi-wavelength laser source

• US 9,407,056 B2
• Filed: 02/09/2015
• Issued: 08/02/2016
• Est. Priority Date: 09/14/2011
• Status: Expired due to Fees

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Xu, Jingzhou, Cho, Gyu
• Primary Examiner(s): Park, Kinam
• Application Number:
  US14/617,028
• Publication Number:
  US 20150180194A1
• Time in Patent Office: 540 Days
• Field of Search: 372/27, 372/26, 372/21, 372/22, 372/6
• US Class Current: 1/1
• CPC Class Codes: G02B 5/3083 Birefringent or phase retarding elements G02B5/3008, G02B5/3016 take precedence; systems for polarisation control G02B27/286; manufacturing phase modulating patterns by lithographic processes G03F7/001
• CPC Class Codes: G02F 1/353 Frequency conversion, i.e. wherein a light beam is generated with frequency components different from those of the incident light beams
• CPC Class Codes: G02F 1/3544 Particular phase matching techniques
• CPC Class Codes: G02F 1/3546 Active phase matching, e.g. by electro- or thermo-optic tuning
• CPC Class Codes: H01S 3/0092 Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity nonlinear frequency conversion per se G02F1/35
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/06712 Polarising fibre; Polariser
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/10053 Phase control
• CPC Class Codes: H01S 3/10061 Polarization control

Abstract

In at least one embodiment a laser system includes a fiber laser source, a polarization controller and a wavelength converter. The relative power distribution between a pump wavelength and a signal wavelength is controllable using the polarization controller. An optional phase compensator is used to control polarization state of the output laser beam. In various embodiments the relative power distribution among multiple wavelengths may be controlled over a range of at least about 100:1.

Claims

1. A laser system, comprising:

a laser source which generates an input beam having a first wavelength;

a polarization controller having one or more polarization controlling components that receive the input beam, the polarization controller controlling a polarization of the input beam;

a wavelength converter which receives the input beam from the polarization controller at a first wavelength and generates a wavelength converted beam in which at least a portion of beam power at the first wavelength is converted into beam power at a second wavelength,

wherein the wavelength converter comprises a polarization sensitive non-linear crystal, wherein the wavelength conversion efficiency is determined by phase matching,

wherein the polarization controller is arranged in such a way that the relative power at each of the first and second wavelengths is controllable, and the laser system output comprises signal power at both the first and second wavelengths, and

an optical phase compensator disposed downstream from the wavelength converter, the optical phase compensator comprising a birefringent optical component and having the same optical axis or parallel optical axis of opposite sign, relative to that of the nonlinear crystal.

2. The laser system of claim 1, wherein the laser source comprises polarization maintaining fiber.

3. The laser system of claim 1, wherein the laser source comprises a pulsed laser that generates a pulsed laser beam having at least one pulse width in the femtosecond to picosecond range.

4. The laser system of claim 1, wherein the polarization controller comprises an electro-optic modulator.

5. The laser system of claim 1, wherein said phase compensator comprises a polarization maintaining fiber, two elements having a prism shape, or a combination thereof.

6. The laser system of claim 1, wherein the laser source comprises one or both of a fiber laser or amplifier.

7. The laser system of claim 1, further comprising a feedback controller to stabilize the output laser power.

8. The laser system of claim 1, wherein the first wavelength is a pump wavelength, the second wavelength is a signal wavelength, and the laser system is configured as a portion of a system for time gating pump and probe measurements, wherein energy at the first wavelength is used to excite an object and energy at the second wavelength is used as a probe.

9. The laser system of claim 1, wherein the laser system is configured as a portion of a material processing system in which energy at the first wavelength is used to pre-process a target material and energy at the second wavelength is used to further process the target material.

10. The laser system of claim 1, wherein the wavelength converter comprises a quasi-phase matched or a non-critical phase matched non-linear crystal, said non-linear crystal characterized by having a wavelength dependent response to temperature.

11. The laser system of claim 10, wherein said quasi-phase matched crystal comprises periodically poled lithium niobate (PPLN).

12. The laser system of claim 10, wherein said non-critical phase matched crystal comprises lithium triborate (LBO).

13. The laser system of claim 1, wherein a wavelength dependent signal power at the output of the wavelength converter can be varied from full available power output to near extinction.

18. The laser system of claim 1, wherein said polarization sensitive non-linear crystal produces a phase delay between the polarization states of light of the first wavelength passing through the crystal .

19. The laser system of claim 1, wherein said birefringent optical component is arranged with a thickness that is set to give the same value of phase delay as the nonlinear crystal while being opposite in sign.

20. The laser system of claim 1, wherein said phase matching comprises quasi-phase matching.

21. The laser system of claim 1, wherein said phase matching comprises non-critical phase matching.

14. A laser system, comprising:

a fiber-based laser source which generates an input beam having a first wavelength;

a polarization controller having one or more polarization controlling components that receive the input beam, the polarization controller controlling a polarization of the input beam;

a wavelength converter which receives the input beam from the polarization controller and generates a wavelength converted beam in which at least a portion of beam power at the first wavelength is converted into beam power at a second wavelength, wherein the polarization controller is arranged in such a way that the relative power at each of the first and second wavelengths is controllable, and the laser system output comprises signal power at both the first and second wavelengths;

wherein the wavelength converter comprises a polarization sensitive non-linear crystal, wherein the wavelength conversion efficiency is determined by phase matching,

an optical phase compensator disposed downstream from the wavelength converter, the optical phase compensator comprising a birefringent optical component and having the same optical axis or parallel optical axis of opposite sign, relative to that of the nonlinear crystal;

and

a spectral selective filter to select either the first wavelength or the second wavelength.

15. The laser system of claim 14, wherein the first wavelength is a pump wavelength, the second wavelength is a signal wavelength, and the laser system is configured as a portion of a system for time gating pump and probe measurements, wherein energy at the first wavelength is used to excite an object and energy at the second wavelength is used as a probe.

16. The laser system of claim 14, wherein the laser system is configured as a portion of a material processing system in which energy at the first wavelength is used to pre-process a target material and energy at the second wavelength is used to further process the target material.

17. The laser system of claim 14, wherein a wavelength dependent signal power at the output of the wavelength converter can be varied from full available power output to near extinction.

22. The laser system of claim 14, wherein said polarization sensitive non-linear crystal produces a phase delay between the polarization states of light of the first wavelength passing through the crystal .

23. The laser system of claim 14, wherein said birefringent optical component is arranged with a thickness that is set to give the same value of phase delay as the nonlinear crystal while being opposite in sign.

24. The laser system of claim 14, wherein said phase matching comprises quasi-phase matching.

25. The laser system of claim 14, wherein said phase matching comprises non-critical phase matching.