Polarization and wavelength stable superfluorescent sources

• US 6,429,965 B1
• Filed: 10/29/1999
• Issued: 08/06/2002
• Est. Priority Date: 11/02/1998
• Status: Expired due to Term

• Current Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford University)
• Original Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford University)
• Inventors: Digonnet, Michel J. F., Falquier, Dario G., Shaw, H. John
• Primary Examiner(s): Tarcza, Thomas H.
• Assistant Examiner(s): Hughes, Deandra M.
• Application Number:
  US09/429,049
• Time in Patent Office: 1,012 Days
• Field of Search: 359/333, 359/341.1, 359/341.3, 359/337, 372/6, 372/27, 372/70, 372/341.33
• US Class Current: 359/341.1
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/06795 with superfluorescent emission, e.g. amplified spontaneous emission sources for fibre laser gyrometers fibre laser gyrometers per se G01C19/72
• CPC Class Codes: H01S 3/094042 of a fibre laser
• CPC Class Codes: H01S 3/09415 the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping

Abstract

The instability of the mean wavelength of a superfluorescent fiber source (SFS) is reduced by randomizing the polarization of light from a pump source or by using polarization maintaining components. In one embodiment, the polarization of a pump source is made more random, leading to greater stability of the mean wavelength of the SFS, with an output mean wavelength that is stable to better than 3 ppm for full rotation of the pump polarization state. In another embodiment, the polarization of optical radiation throughout the device is kept substantially constant by using polarization maintaining fiber and components, thereby leading to enhanced mean wavelength stability of the SFS.

Claims

1. A superfluorescent source, comprising:

an optical pump source generating optical radiation that is substantially unpolarized; and

a solid state laser medium that is pumped by the substantially unpolarized optical radiation, said medium having characteristics selected to generate superfluorescence having a full width at half maximum (FWHM) of at least 2 nm and a mean wavelength that is stable to within 50 ppm against polarization fluctuations in said superfluorescent source.

2. The superfluorescent source of claim 1, wherein the superfluorescence from said medium is generated by rare earth ions.

3. The superfluorescent source of claim 1, wherein the superfluorescence from said medium is generated by erbium ions.

4. The superfluorescent source of claim 3, comprising an optical coupling element that couples the optical radiation to said medium.

5. The superfluorescent source of claim 4, wherein said optical coupling element is a wavelength division multiplexing (WDM) coupler.

6. The superfluorescent source of claim 1, comprising an isolator to reduce optical feedback.

7. The superfluorescent source of claim 3, further comprising a fiber optic gyroscope, wherein the superfluorescence of said superfluorescent source is input into said gyroscope.

8. The superfluorescent source of claim 3, wherein said optical pump source comprises:

a laser; and

a depolarizer.

9. The superfluorescent source of claim 8, wherein said depolarizer is a Lyot depolarizer.

10. The superfluorescent source of claim 8, wherein said depolarizer includes a PZT modulator.

11. The superfluorescent source of claim 8, further comprising a second depolarizer on the output side of said laser medium.

12. The superfluorescent source of claim 1, wherein the superfluorescence has a mean wavelength that is stable to within 3 ppm against fluctuations in said superfluorescent source.

13. The superfluorescent source of claim 8, wherein said laser includes a laser diode.

14. The superfluorescent source of claim 1, wherein said solid state medium comprises an optical waveguide.

15. The superfluorescent source of claim 1, wherein said solid state medium comprises an optical fiber.

16. The superfluorescent source of claim 1, wherein the mean wavelength is stable to within 50 ppm against birefringence changes in said superfluorescent source.

17. The superfluorescent source of claim 1, wherein the mean wavelength is stable to within 50 ppm against polarization changes of the optical radiation from said optical pump source.

18. The superfluorescent source of claim 1, said optical pump source comprising a plurality of pumps, said plurality of pumps having outputs with polarizations selected such that the optical radiation from said optical pump source is substantially unpolarized.

19. The superfluorescent source of claim 18, wherein said plurality of pumps includes two pumps whose respective optical outputs are combined so that the polarizations of the outputs are orthogonal to each other.

20. A superfluorescent source, comprising:

an optical pump source generating optical radiation that is substantially unpolarized; and

a solid state laser medium that is pumped by the substantially unpolarized optical radiation, said medium having characteristics selected to generate superfluorescence having a full width at half maximum (FWHM) of at least 2 nm and a mean wavelength that is stable to within 50 ppm against polarization changes in said source that range over the Poincaire sphere.

21. A superfluorescent source, comprising:

an optical pump source generating optical radiation that is substantially unpolarized, said optical pump source including;

a plurality of pumps that generate respective optical outputs;

a polarization mixer that receives the respective optical outputs from said plurality of pumps and generates optical output, wherein the respective optical outputs from said plurality of pumps have polarizations selected such that optical output from said mixer is substantially unpolarized; and

a depolarizer that receives the optical output from said polarization mixer; and

a solid state laser medium that is pumped by the output from said depolarizer, said medium having characteristics selected to generate superfluorescence having a full width at half maximum (FWHM) of at least 2 nm and a mean wavelength that is stable against polarization fluctuations in said superfluorescent source.

23. The superfluorescent source of claim 21, wherein the mean wavelength is stable to within 500 ppm against polarization fluctuations in said superfluorescent source.

24. The superfluorescent source of claim 21, wherein the mean wavelength is stable to within 100 ppm against polarization fluctuations in said superfluorescent source.

25. The superfluorescent source of claim 21, wherein the mean wavelength is stable to within 50 ppm against polarization fluctuations in said superfluorescent source.

26. The superfluorescent source of claim 21, wherein the mean wavelength is stable to within 3 ppm against polarization fluctuations in said superfluorescent source.

27. The superfluorescent source of claim 21, wherein said plurality of pumps includes two pumps having respective optical outputs combined so that the polarizations of the outputs are orthogonal to each other.

28. The superfluorescent source of claim 21, wherein the superfluorescence from said medium is generated by erbium ions.

29. The superfluorescent source of claim 21, wherein the superfluorescence from said laser medium is generated by rare earth ions.

30. The superfluorescent source of claim 21, comprising an isolator to reduce optical feedback.

31. The superfluorescent source of claim 21, further comprising a fiber optic gyroscope, wherein the superfluorescence of said superfluorescent source is input into said gyroscope.

32. The superfluorescent source of claim 21, wherein said plurality of pumps comprise lasers.

33. The superfluorescent source of claim 21, wherein said depolarizer is a Lyot depolarizer.

34. The superfluorescent source of claim 21, wherein said depolarizer includes a PZT modulator.

35. The superfluorescent source of claim 21, wherein said solid state medium comprises an optical waveguide.

36. The superfluorescent source of claim 21, wherein said solid state medium comprises an optical fiber.

37. The superfluorescent source of claim 21, wherein the mean wavelength is stable to within 500 ppm against birefringence changes in said superfluorescent source.

38. The superfluorescent source of claim 21, wherein the mean wavelength is stable to within 500 ppm against polarization changes of the optical radiation from said optical pump source.

39. The superfluorescent source of claim 21, further comprising a dichroic reflector between said depolarizer and said medium, said reflector reflecting backward traveling optical radiation from said medium back through said medium.

22. The superfluorescent source of 21, further comprising a dichroic reflector between said depolarizer and said medium.

40. A method of generating superfluorescence, comprising:

providing a plurality of optical pumps, the pumps having respective optical outputs with different polarizations;

directing the respective optical outputs through a polarization mixer that produces optical output, wherein the different polarizations are selected so that the optical output from the mixer is substantially unpolarized;

depolarizing the output from the mixer;

injecting the depolarized output into a solid state laser medium; and

producing superfluorescence from the medium that has a mean wavelength that is stable against polarization fluctuations in the superfluorescent source.

41. The method of claim 40, wherein the wavelength is stable to within 500 ppm against polarization fluctuations in said superfluorescent source.

42. The method of claim 40, wherein the superfluorescence has a full width at half maximum (FWHM) of at least 2 nm.

43. The method of claim 40, wherein said depolarizing includes directing the output from the mixer through a depolarizer.

44. The method of claim 40, wherein the plurality of optical pumps includes two pumps having respective optical outputs whose polarizations are orthogonal to each other.

45. The method of claim 40, wherein the solid state medium includes rare earth ions.