Method and apparatus for spectral-beam combining of fanned-in laser beams with chromatic-dispersion compensation using a plurality of diffractive gratings

• US 8,179,594 B1
• Filed: 06/30/2008
• Issued: 05/15/2012
• Est. Priority Date: 06/29/2007
• Status: Active Grant

• Current Assignee: Lockheed Martin Corporation (Martin Marietta Corporation)
• Original Assignee: Lockheed Martin Corporation (Martin Marietta Corporation)
• Inventors: Tidwell, Steven C., Loftus, Thomas H., Lemaire, Charles A.
• Primary Examiner(s): BOLDA, ERIC L
• Application Number:
  US12/165,651
• Time in Patent Office: 1,415 Days
• Field of Search: 359/349
• US Class Current: 359/349
• CPC Class Codes: H01S 3/005 Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping shaping laser beam for working metal or other materials B23K26/06; optical elements, systems or apparatus in general G02B
• CPC Class Codes: H01S 3/2391 emitting at different wavelengths
• CPC Class Codes: H04B 10/2513 due to chromatic dispersion

Abstract

Apparatus and method for spectral-beam combining of light from a plurality of high-power lasers (e.g., fiber MOPA lasers) that, in some embodiments, use substantially identical diffraction gratings in a 1-D non-parallel, mutually compensating configuration to combine non-parallel converging input beams in one plane each having a slightly different successively higher wavelength into a single output beam of high quality. In other embodiments, an output grating and one or more input gratings in a 1-D parallel, mutually compensating configuration combine non-parallel input beams in one plane into a single output beam of high quality. In other embodiments, a 2-D plurality of input gratings in a non-parallel configuration combine a plurality of non-parallel input beams not in one plane each having a slightly different successively higher wavelength into a set of converging beams in one plane directed towards an output grating that compensates for chromatic dispersions introduced by the input gratings.

Claims

1. A method comprising:

providing a plurality of laser beams including a first laser beam at a first characteristic wavelength and a second laser beam at a second characteristic wavelength;

providing a diffractive output grating;

providing one or more diffractive input gratings optically coupled to receive the first and second laser beams, wherein the first and second laser beams are non parallel to one another when they impinge on the one or more input gratings;

diffracting the first and second laser beams with the one or more input gratings at converging angles toward the output grating; and

spectrally combining the first and second laser beams into a single output beam at the output grating.

2. The method of claim 1, further comprising:

placing the one or more input gratings all parallel to one another and substantially parallel to the output grating with the faces of the input gratings facing the grating face of the output grating, and wherein the one or more input gratings each have a grating-line spacing that is different than the output grating'"'"'s grating-line spacing.

3. The method of claim 1, further comprising:

placing the one or more input gratings each non-parallel to the output grating with the faces of the input gratings generally facing the output grating, and wherein the one or more input gratings each have a grating-line spacing that is equal to the output grating'"'"'s grating-line spacing.

4. The method of claim 1, further comprising:

generating the plurality of laser beams with master-oscillator power-amplifier (MOPA) laser sources having fiber gain media.

5. The method of claim 1, wherein the spectrally combining outputs the single output beam at a power/area of at least about 10,000 W/(cm² of grating surface of the output grating).

6. The method of claim 1, wherein the spectrally combining outputs the single output beam at a power of at least about 10 megawatts.

7. The method of claim 1, wherein the diffracting the first and second laser beams with the one or more input gratings includes introducing a first chromatic dispersion to the first laser beam and a second chromatic dispersion to the second laser beam, and wherein the spectrally combining of the first and second laser beams includes introducing an opposite chromatic dispersion that negates at least a portion of the first chromatic dispersion and at least a portion of the second chromatic dispersion such that the output beam has less chromatic dispersion than either the first or the second laser beams after they encounter the one or more input gratings.

8. The method of claim 7, wherein the first chromatic dispersion'"'"'s angle of dispersion is substantially equal to the second chromatic dispersion'"'"'s angle of dispersion.

9. The method of claim 7, wherein a diameter of the first beam due to the first chromatic dispersion'"'"'s dispersion at the output grating is substantially equal to a corresponding diameter of the second beam due to the second chromatic dispersion'"'"'s dispersion at the output grating.

10. The method of claim 1, wherein the one or more input gratings include a plurality of input gratings, the method further comprising:

locating each of the plurality of input gratings approximately equidistant from the output grating.

11. An apparatus comprising:

a plurality of laser sources configured to emit laser beams including a first laser beam at a first characteristic wavelength and a second laser beam at a second characteristic wavelength;

a diffractive output grating; and

one or more diffractive input gratings optically coupled to the plurality of laser sources to receive the first and second laser beams, wherein the first and second laser beams are non parallel to one another, and wherein the one or more input gratings diffract the first and second laser beams at converging angles toward the output grating; and

wherein the output grating is configured to spectrally combine the first and second laser beams into a single output beam.

12. The apparatus of claim 11, wherein the one or more input gratings are all parallel to one another and substantially parallel to the output grating with the faces of the input gratings facing the grating face of the output grating, and wherein the one or more input gratings each have a grating-line spacing that is different than the output grating'"'"'s grating-line spacing.

13. The apparatus of claim 11, wherein the one or more input gratings are each non-parallel to the output grating with the faces of the input gratings generally facing the output grating, and wherein the one or more input gratings each have a grating-line spacing that is equal to the output grating'"'"'s grating-line spacing.

14. The apparatus of claim 11, wherein the plurality of laser sources include one or more master-oscillator power-amplifier (MOPA) laser sources having fiber gain media.

15. The apparatus of claim 11, wherein the single output beam outputs at a power/area of at least about 10,000 W/(cm² of grating surface of the output grating).

16. The apparatus of claim 11, wherein the single output beam has a power of at least about 10 megawatts.

17. The apparatus of claim 11, wherein the one or more input gratings are configured to introduce a first chromatic dispersion to the first laser beam and a second chromatic dispersion to the second laser beam, and wherein the output grating introduces an opposite chromatic dispersion that negates at least a portion of the first chromatic dispersion and at least a portion of the second chromatic dispersion such that the output beam has less chromatic dispersion than either the first or the second laser beams after they encounter the one or more input gratings.

18. The apparatus of claim 17, wherein the first chromatic dispersion'"'"'s angle of dispersion is substantially equal to the second chromatic dispersion'"'"'s angle of dispersion.

19. The apparatus of claim 17, wherein a diameter of the first beam due to the first chromatic dispersion'"'"'s dispersion at the output grating is substantially equal to a corresponding diameter of the second beam due to the second chromatic dispersion'"'"'s dispersion at the output grating.

20. The apparatus of claim 11, wherein the one or more input gratings include a plurality of input gratings that are each placed approximately equidistant from the output grating.

21. The apparatus of claim 11, wherein at least some of the one or more input gratings are high-efficiency dielectric gratings.

22. The apparatus of claim 11, wherein the output grating is a high-efficiency dielectric grating.

23. An apparatus comprising:

a plurality of fiber gain media configured to emit laser beams including a first fiber gain medium that emits a first laser beam at a first characteristic wavelength having a full-width half maximum (FWHM) linewidth of at most 1 nm and a second fiber gain medium that emits a second laser beam, non-parallel to the first beam, at a second characteristic wavelength having an FWHM linewidth of at most 1 nm; and

means for spectrally combining and chromatic-dispersion compensating the first and second non-parallel laser beams into a single output beam.