IP Library Granted Patent US 7,880,961
Granted Patent B1
US 7,880,961 · App. 11/800,383 · Granted Feb 1, 2011

Optical amplifier exhibiting net phase-mismatch selected to at least partially reduce gain-induced phase-matching during operation and method of operation

Assignee: Sandia Corporation
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Quick Facts
Patent No.
US 7,880,961
App. No.
11/800,383
Granted
Feb 1, 2011
Kind
B1
Abstract

An optical amplifier, such as an optical waveguide amplifier (e.g., an optical fiber amplifier or a planar waveguide) or a non-guiding optical amplifier, that exhibits a net phase-mismatch selected to at least partially reduce gain-induced phase-matching during operation thereof is disclosed. In one aspect of the invention, an optical amplifier structure includes at least one optical amplifier having a length and a gain region. The at least one optical amplifier exhibits a net phase-mismatch that varies along at least part of the length thereof selected to at least partially reduce gain-induced phase-matching during operation thereof.

Claims (58)

1. An optical amplifier structure, comprising:

at least one optical amplifier including a length and a gain region;

wherein the at least one optical amplifier exhibits a net phase-mismatch that varies along at least part of the length thereof selected to at least partially reduce gain-induced phase-matching during operation thereof, the net phase-mismatch being controlled by longitudinally varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the at least one optical amplifier.

2. The optical amplifier structure of claim 1 wherein the at least one optical amplifier is configured as an optical waveguide amplifier.

3. The optical amplifier structure of claim 1 wherein the at least one optical amplifier is configured as an optical fiber amplifier.

4. The optical amplifier structure of claim 1 wherein the at least one optical amplifier is configured as an optical fiber laser.

5. The optical amplifier structure of claim 1 wherein the net phase-mismatch is controlled by varying the modal dispersion of the at least one optical amplifier along the at least part of the length thereof.

6. The optical amplifier structure of claim 1 wherein the net phase-mismatch is controlled by coiling at least a portion of the at least one optical amplifier.

7. The optical amplifier structure of claim 6 wherein:

the at least one optical amplifier is configured as an optical fiber amplifier; and

the at least a portion of the optical fiber amplifier is coiled with a bend radius that varies along the at least part of the length thereof.

8. The optical amplifier structure of claim 6 wherein:

the at least one optical amplifier is configured as an optical fiber amplifier; and

the at least a portion of the optical fiber amplifier comprises a first portion that is coiled with a first bend radius and a second portion that is coiled with a second bend radius that is not equal to the first bend radius.

9. The optical amplifier structure of claim 6 wherein:

the at least one optical amplifier is configured as an optical fiber amplifier; and

the at least a portion of the optical fiber amplifier comprises a first coiled portion, a second coiled portion, and an uncoiled portion therebetween.

10. The optical amplifier structure of claim 1 wherein the at least one optical amplifier is structured to provide the net phase-mismatch that varies along the at least part of the length thereof.

11. The optical amplifier structure of claim 10 wherein the at least one optical amplifier comprises a core having a lateral dimension that varies along the at least part of the length thereof.

12. The optical amplifier structure of claim 1 wherein the at least one optical amplifier is configured as a holey fiber.

13. The optical amplifier structure of claim 1 wherein the net phase mismatch is provided by a stress field that varies along the at least part of the length of the at least one optical amplifier.

14. The optical amplifier structure of claim 1 wherein the net phase-mismatch is controlled by varying the material dispersion of the at least one optical amplifier along the at least part of the length thereof.

15. The optical amplifier structure of claim 1 wherein the net phase-mismatch is provided by a temperature gradient along the at least part of the length of the at least one optical amplifier.

16. The optical amplifier structure of claim 1 wherein the at least one optical amplifier comprises a plurality of optical fiber amplifiers that are spliced together, each of the plurality of optical fiber amplifiers having a core region that exhibits different respective indices of refractions.

17. The optical amplifier structure of claim 1 wherein the at least one optical amplifier comprises a transverse refractive index profile that varies along the at least part of the length of the at least one optical amplifier to control the net phase-mismatch.

18. The optical amplifier structure of claim 1 wherein the at least one optical amplifier comprises at least one Bragg grating configured to provide the net phase-mismatch that varies along the at least part of the length thereof.

19. The optical amplifier structure of claim 1 , further comprising a device operable to apply one of a stress field, a temperature gradient, or an electric field that varies along the at least part of the length of the at least one optical amplifier to control the net phase-mismatch.

20. The optical amplifier structure of claim 1 wherein the net phase-mismatch substantially reduces gain-induced phase-matching during operation of the at least one optical amplifier.

21. The optical amplifier structure of claim 1 wherein the net phase-mismatch is controlled by varying the nonlinear phase mismatch of the at least one optical amplifier along the at least part of the length thereof.

22. The optical amplifier structure of claim 21 wherein the nonlinear phase mismatch is varied by longitudinally varying the concentration of active elements present in the gain region of the at least one optical amplifier.

23. The optical amplifier structure of claim 21 wherein the nonlinear phase mismatch is varied by longitudinally varying the nonlinear index of refraction of the at least one optical amplifier.

24. The optical amplifier structure of claim 21 wherein:

the at least one optical amplifier is configured as an optical fiber amplifier that comprises an inner cladding disposed between a core including the gain region and an outer cladding; and

the nonlinear phase mismatch is varied by longitudinally varying the geometry of the inner cladding.

25. The optical amplifier structure of claim 21 wherein the at least one optical amplifier comprises a plurality of optical fiber amplifiers that are spliced together, each of the plurality of optical fiber amplifiers having a core region that exhibit different respective nonlinear indices of refractions.

26. The optical amplifier structure of claim 21 wherein the at least one optical amplifier is configured to allow light output from a pump for exciting the gain region to be input at multiple locations along the length of the at least one optical amplifier.

27. The optical amplifier structure of claim 1 wherein the net phase-mismatch is present in the at least one optical amplifier when the at least one optical amplifier is not in operation.

28. A method for reducing gain-induced phase-matching in an optical amplifier having a length, comprising:

varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length; and

at least partially reducing gain-induced phase-matching in the optical amplifier during operation thereof as a result of the variation in the net phase-mismatch.

29. The method of claim 28 wherein the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length varying the modal dispersion of the optical amplifier along the at least part of the length thereof.

30. The method of claim 28 wherein:

the optical amplifier is configured as an optical fiber amplifier; and

the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length comprises coiling the optical fiber amplifier to exhibit a non-uniform bend radius along the at least part of the length thereof.

31. The method of claim 28 wherein:

the optical amplifier is configured as an optical fiber amplifier; and

the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length coiling discrete portions of the optical fiber amplifier to exhibit different respective bend radii.

32. The method of claim 28 wherein the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length providing a core to the optical amplifier that has a lateral dimension that varies along the at least part of the length thereof.

33. The method of claim 28 wherein the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length varying the material dispersion of the optical amplifier along the at least part of the length thereof.

34. The method of claim 28 wherein the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length comprises applying a stress to the optical amplifier that varies along the at least part of the length thereof.

35. The method of claim 28 wherein the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length applying a temperature gradient along the at least part of the length of the optical amplifier.

36. The method of claim 28 wherein the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length applying an electric field that varies along the at least part of the length of the optical amplifier.

37. The method of claim 28 wherein the act of providing the optical amplifier with a net phase-mismatch that varies along at least part of the length thereof varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length splicing a plurality of optical fiber amplifiers together, each of the optical fiber amplifiers having different respective core index of refractions.

38. The method of claim 28 wherein the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length comprises exposing the optical amplifier to ultraviolet light to impart a selected variation in the index of refraction of the optical amplifier.

39. The method of claim 28 wherein the act of varying at least one of material dispersion, modal dispersion, or nonlinear phase-mismatch of the optical amplifier so that the net phase-mismatch varies along at least part of the length varying the nonlinear phase-mismatch of the optical amplifier along the at least part of the length thereof.

40. The method of claim 28 wherein the optical amplifier is configured as an optical waveguide amplifier.

41. The method of claim 28 wherein the optical amplifier is configured as an optical fiber amplifier.

42. The method of claim 28 wherein the optical amplifier is configured as an optical fiber laser.

Assignments (3)
CHANGE OF NAME Recorded Sep 27, 2018
From: SANDIA CORPORATION
To: NATIONAL TECHNOLOGY & ENGINEERING SOLUTIONS OF SANDIA, LLC
Reel/Frame 047157/0622 →
CONFIRMATORY LICENSE Recorded Aug 9, 2007
From: SANDIA CORPORATION
To: ENERGY, U.S. DEPARTMENT OF
Reel/Frame 019671/0976 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jun 27, 2007
From: FARROW, ROGER L.; FEVE, JEAN-PHILIPPE; KLINER, DAHV A.V.
To: SANDIA NATIONAL LABORATORIES
Reel/Frame 019491/0852 →
Continuity (1)
Provisional Application 6083953900 · Aug 22, 2006