High-power, phase-locked, laser arrays

• US 8,340,150 B2
• Filed: 05/23/2011
• Issued: 12/25/2012
• Est. Priority Date: 02/03/2005
• Status: Active Grant

• Current Assignee: Necsel Intellectual Property Inc. (Ushio Incorporated)
• Original Assignee: PD-LD Incorporated (Ushio Incorporated)
• Inventors: Volodin, Boris Leonidovich
• Primary Examiner(s): Zhang, Yuanda
• Application Number:
  US13/113,976
• Publication Number:
  US 20120027035A1
• Time in Patent Office: 582 Days
• Field of Search: 372/29.014, 372/29.016, 372/29.023, 372/50.11, 372/50.12, 372/50.123, 372/99, 372/102, 359/27, 359/337.21, 359/349, 359/583
• US Class Current: 372/50.123
• CPC Class Codes: H01S 3/1305 Feedback control systems
• CPC Class Codes: H01S 5/005 Optical components external to the laser cavity, specially adapted therefor, e.g. for homogenisation or merging of the beams or for manipulating laser pulses, e.g. pulse shaping H01S5/026, H01S5/18388 take precedence
• CPC Class Codes: H01S 5/065 Mode locking; Mode suppression; Mode selection ; Self pulsating
• CPC Class Codes: H01S 5/0654 Single longitudinal mode emission
• CPC Class Codes: H01S 5/141 using a wavelength selective device, e.g. a grating or etalon H01S5/146 takes precedence
• CPC Class Codes: H01S 5/148 using a Talbot cavity
• CPC Class Codes: H01S 5/4012 Beam combining, e.g. by the use of fibres, gratings, polarisers, prisms
• CPC Class Codes: H01S 5/4062 with an external cavity or using internal filters, e.g. Talbot filters
• CPC Class Codes: H01S 5/4068 with lateral coupling by axially offset or by merging waveguides, e.g. Y-couplers

Abstract

High-power, phased-locked, laser arrays as disclosed herein utilize a system of optical elements that may be external to the laser oscillator array. Such an external optical system may achieve mutually coherent operation of all the emitters in a laser array, and coherent combination of the output of all the lasers in the array into a single beam. Such an “external gain harness” system may include: an optical lens/mirror system that mixes the output of all the emitters in the array; a holographic optical element that combines the output of all the lasers in the array, and an output coupler that selects a single path for the combined output and also selects a common operating frequency for all the coupled gain regions.

Claims

1. A method for producing mutually-coherent operation of a plurality of light emitters, each of the emitters outputting a respective power and brightness, the method comprising:

mixing respective beams received from each of the plurality of emitters;

combining the mixed beams in a beam-combining element to form a composite beam containing a respective contribution from each of the emitters; and

feeding back through the beam-combining element at least a portion of the light containing the respective contribution from each of the emitters, the portion having a selected wavelength,

wherein the portion is fed back into the emitters in such a way that each of the emitters receives narrowband light from every other emitter, and

wherein mutually coherent operation of the plurality of emitters is achieved such that each of the emitters lases at the selected wavelength with a phase difference that results in a coherent output beam that effectively combines the powers from each of the emitters such that the output beam has a brightness that is greater than the brightnesses of the individual emitters.

2. The method of claim 1, further comprising:

mixing the beams received from the emitters by overlapping the received beams in a focal plane of a lens.

3. The method of claim 2, wherein the lens performs an optical Fourier transform on the beams received from the emitters.

4. The method of claim 2, wherein the beam-combining element is positioned in the focal plane of the lens.

5. The method of claim 4, wherein the beam-combining element is a diffractive optical element.

6. The method of claim 4, wherein the beam-combining element is a digital optical element.

7. The method of claim 4, wherein the beam-combining element is a holographic optical element.

8. The method of claim 2, wherein the beam-combing element is positioned in a focal plane of a second lens.

9. The method of claim 1, further comprising:

allowing the composite beam to pass through a path selector.

10. The method of claim 9, wherein an output coupler reflects at least a portion of the composite beam back through the path selector.

11. The method of claim 10, wherein the output coupler comprises a three-dimensional optical element having a Bragg grating recorded holographically therein.

12. The method of claim 11, wherein the Bragg grating is a reflective Bragg grating.

13. The method of claim 11, wherein the Bragg grating is a transmissive Bragg grating.

14. The method of claim 10, wherein the output coupler comprises a phase-conjugate mirror.

15. The method of claim 10, wherein the output coupler comprises a diffraction grating.

16. The method of claim 10, wherein the output coupler is a tunable output coupler that provides for wavelength tuning of the reflected portion of the composite beam.

17. The method of claim 16, wherein the tunable output coupler provides for the wavelength tuning via angular adjustment of the output coupler.

18. The method of claim 1, wherein the respective contributions from each of the emitters are received by a three-dimensional optical element.

19. The method of claim 18, wherein the composite beam is created via an optical method that includes the three-dimensional optical element.

20. The method of claim 19, wherein the composite beam is created via an optical method that includes the three-dimensional optical element receiving the beams from the emitters and forming the composite beam containing the respective contributions from each of the emitters.