Non-Circular Optical Fiber and Mode Shape Converter and Method

• US 20200132925A1
• Filed: 07/05/2018
• Published: 04/30/2020
• Est. Priority Date: 07/06/2017
• Status: Active Grant

• Current Assignee: Lawrence Livermore National Security LLC (Government of the United States of America)
• Original Assignee: Lawrence Livermore National Security LLC (Government of the United States of America)
• Inventors: Drachenberg, Derrek R., Alien, Graham S., Chen, Diana C., Cook, Matthew J., Crist, Robert P., Dawson, Jay W., Kiani, Leily, Messerly, Michael J., Pax, Paul H., Schenkel, Nick, Yu, Charles X., Khitrov, Victor V.
• Granted Patent: US 11,340,396 B2
• Time in Patent Office: Days
• CPC Class Codes: G02B 2006/1209 Multimode
• CPC Class Codes: G02B 2006/12102 Lens
• CPC Class Codes: G02B 2006/12121 Laser
• CPC Class Codes: G02B 6/0288 Multimode fibre, e.g. graded index core for compensating modal dispersion
• CPC Class Codes: G02B 6/12 of the integrated circuit kind electric integrated circuits H01L27/00
• CPC Class Codes: G02B 6/1228 Tapered waveguides, e.g. integrated spot-size transformers for coupling with fibres G02B6/305
• CPC Class Codes: G02B 6/14 Mode converters
• CPC Class Codes: G02B 6/4202 for coupling an active element with fibres without intermediate optical elements, e.g. fibres with plane ends, fibres with shaped ends, bundles

Abstract

A class of fibers is described that have a non-circular cross section on one or both ends that can by optimized to capture the optical radiation from a laser diode or diode array and deliver the light in the same or different shape on the opposite end of the fiber. A large multimode rectangular waveguide may be provided which can accept the radiation from a high-power diode bar and transform it into a circular cross section on the opposite end, while preserving brightness.

Claims

1. An apparatus, comprising:

a multimode central waveguide having a first index of refraction n₁ and having an input aperture and an output aperture, wherein said input aperture is non-circular and larger than an input laser beam directed into said input aperture, wherein said input laser beam at said input aperture produces an input brightness and an input spatial and angular distribution; and

a cladding surrounding said central waveguide, wherein said cladding has a second index of refraction n₂, wherein n₁>

n₂, wherein said central waveguide and said cladding together comprise a taper along their length that redistributes said input spatial and angular distribution to produce a redistributed spatial and angular distribution at said output aperture and maintains at least 90% of said input brightness at said output aperture.

2. The apparatus of claim 1, wherein said taper maintains one of at least 95% of said input brightness at said output aperture or at least 99% of said input brightness at said output aperture.

4. The apparatus of claim 1, wherein said multimode central waveguide will support one of at least 100 modes or at least 10,000 modes.

6. The apparatus of claim 1, wherein said cladding is in direct contact with said central waveguide.

7. The apparatus of claim 1, further comprising a laser for providing said laser beam, wherein said laser beam has a non-circular cross-section.

8. The apparatus of claim 1, wherein said input aperture has a rectangular cross-section, wherein said output aperture has a circular cross-section and wherein said cladding is in direct contact with said waveguide.

9. The apparatus of claim 8, wherein said input aperture has an angular distribution that is greater than that of the input laser beam.

11. The apparatus of claim 1, wherein said laser beam comprises a fast axis and a slow axis, the apparatus further comprising a cylindrical lens and at least one of a focusing lens or a focusing lens pair, wherein said cylindrical lens is configured to act on said fast axis so that it matches the divergence angle between said fast axis and said slow axis and wherein said focusing lens or said focusing lens pair is configured to then focus said laser beam onto said input aperture.

13. The apparatus of claim 1, wherein said taper is long enough to make said redistributed spatial and angular distribution to be adiabatic.

14. The apparatus of claim 1, wherein said taper provides a reduction in diameter of said waveguide of a least 50%.

15. The apparatus of claim 1, further comprising a peripheral waveguide surrounding and in direct contact with said central waveguide, wherein said cladding surrounds and is in direct contact with said peripheral waveguide, wherein said peripheral waveguide comprises a third index of refraction n₃, wherein n₁>

n₃>

n₂.

16. The apparatus of claim 15, wherein said input aperture has a rectangular cross-section and wherein said peripheral waveguide has a circular cross-section at said input aperture and at said output aperture.

17. The apparatus of claim 16, wherein said input aperture has a spatial distribution and an angular distribution that are both greater than that of the input laser beam.

18. The apparatus of claim 1, further comprising a laser for providing said laser beam, wherein said laser beam has a rectangular cross-section, wherein said laser beam comprises a fast axis and a slow axis, the apparatus further comprising a cylindrical lens and one of a focusing lens or a focusing lens pair, wherein said cylindrical lens is configured to act on said fast axis so that it matches the divergence angle between said fast axis and said slow axis and wherein said focusing lens or focusing lens pair is configured to then focus said laser beam onto said input aperture.

23. The apparatus of claim 16, wherein said taper is configured such that said input brightness will couple out into said peripheral core by the time it reaches said output aperture.

3. (canceled)

5. (canceled)

10. (canceled)

12. (canceled)

19-22. -22. (canceled)

24. A method, comprising:

providing an apparatus including (i) a multimode central waveguide having a first index of refraction n₁ and having an input aperture and an output aperture, wherein said input aperture is non-circular and larger than an input laser beam directed into said input aperture, wherein said input laser beam at said input aperture produces an input brightness and an input spatial and angular distribution; and

(ii) a cladding surrounding said central waveguide, wherein said cladding has a second index of refraction n₂, wherein n₁>

n₂, wherein said central waveguide and said cladding together comprise a taper along their length that redistributes said input spatial and angular distribution to produce a redistributed spatial and angular distribution at said output aperture and maintains at least 90% of said input brightness at said output aperture; and

directing said input laser beam into said input aperture, wherein said taper redistributes said input spatial and angular distribution to produce said redistributed spatial and angular distribution at said output aperture and maintains at least 90% of said input brightness at said output aperture.

25. The method of claim 24, wherein said taper maintains one of at least 95% of said input brightness at said output aperture or at least 99% of said input brightness at said output aperture.

27. The method of claim 24, wherein said multimode central waveguide will support one of at least 100 modes or at least 10,000 modes.

29. The method of claim 24, wherein said cladding is in direct contact with said waveguide.

30. The method of claim 24, further comprising providing a laser for providing said laser beam, wherein said laser beam has a non-circular cross-section

31. The method of claim 24, wherein said input aperture has a rectangular cross-section, wherein said output aperture has a circular cross-section and wherein said cladding is in direct contact with said waveguide.

32. The method of claim 31, wherein said input aperture has an angular distribution that is greater than that of the input laser beam.

34. The method of claim 24, wherein said laser beam comprises a fast axis and a slow axis, the method further comprising providing a cylindrical lens at least one of and a focusing lens or a focusing lens pair, wherein said cylindrical lens is configured to act on said fast axis so that it matches the divergence angle between said fast axis and said slow axis and wherein said focusing lens or said focusing lens pair is configured to then focus said laser beam onto said input aperture.

36. The method of claim 24, wherein said taper is long enough to make said redistributed spatial and angular distribution to be adiabatic.

37. The method of claim 24, wherein said taper provides a reduction in diameter of said waveguide of a least 50%.

38. The method of claim 24, wherein said apparatus further comprises a peripheral waveguide surrounding and in direct contact with said central waveguide, wherein said cladding surrounds and is in direct contact with said peripheral waveguide, wherein said peripheral waveguide comprises a third index of refraction n₃, wherein n₁>

n₃>

n₂.

39. The method of claim 38, wherein said input aperture has a rectangular cross-section and wherein said peripheral waveguide has a circular cross-section at said input aperture and at said output aperture.

40. The method of claim 39, wherein said input aperture has a spatial distribution and an angular distribution that are both greater than that of the input laser beam.

41. The method of claim 24, further comprising a laser for providing said laser beam, wherein said laser beam has a rectangular cross-section, wherein said laser beam comprises a fast axis and a slow axis, the apparatus further comprising a cylindrical lens and one of a focusing lens or a focusing lens pair, wherein said cylindrical lens is configured to act on said fast axis so that it matches the divergence angle between said fast axis and said slow axis and wherein said focusing lens or focusing lens pair is configured to then focus said laser beam onto said input aperture.

46. The method of claim 39, wherein said taper is configured such that said input brightness will couple out into said peripheral core by the time it reaches said output aperture.

26. (canceled)

28. (canceled)

33. (canceled)

35. (canceled)

42-45. -45. (canceled)