Fiber optic inter-mode coupling single side band frequency shifter

• US 4,832,437 A
• Filed: 05/11/1987
• Issued: 05/23/1989
• Est. Priority Date: 01/17/1986
• Status: Expired due to Term

• Current Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Original Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Inventors: Blake, James N., Engan, Helege E., Shaw, Herbert J., Kim, Byoung Y.
• Primary Examiner(s): Sikes, William L.
• Assistant Examiner(s): Ullah, Akm E.
• Application Number:
  US07/048,142
• Time in Patent Office: 743 Days
• Field of Search: 350/96.15, 350/96.29, 350/96.30, 250/227
• US Class Current: 385/1
• CPC Class Codes: G02B 6/14 Mode converters
• CPC Class Codes: G02B 6/2821 using lateral coupling between contiguous fibres to split or combine optical signals
• CPC Class Codes: G02F 1/0134 in optical waveguides

Abstract

An optical fiber is subjected to a series of traveling flexural waves propagating along a length of the fiber. At least a portion of an optical signal propagating within the optical fiber in a first propagation mode is coupled to a second propagation mode. The optical signal in the second propagation mode has a frequency which is equal to either the sum of or the difference between the frequency of the optical signal in the first propagation mode and the frequency of the traveling flexural waves. The frequency of the optical signal in the second propagation mode is shifted upward or downward from the frequency of the optical signal in the first propagation mode as determined by the direction of propagation of the first optical signal with respect to the direction of propagation of the traveling flexural waves, and as also determined by whether the phase propagation velocity of the optical signal in the first propagation mode is greater than or less than the propagation velocity of the optical signal in the second propagation mode.

Claims

1. An apparatus for coupling light between optical propagation modes in an optical fiber, comprising:

an optical fiber having a first optical propagation mode and a second optical propagation mode for light propagating therein; and

a generator, connected to said fiber such that said generator produces a flexural wave which propagates in said optical fiber, the energy of said flexural wave confined to said optical fiber, said flexural wave having a frequency, a propagation velocity and a wavelength, said wavelength of said flexural wave being a function of said frequency and said propagation velocity, and being selected to cause coupling of light from one of said first an secon moes to the other of said first an secon moes.

2. The apparatus as defined in claim 1, wherein the propagation velocity of said flexural wave is dependent upon the cross sectional dimensions of said fiber and wherein said cross-sectional dimensions vary along said fiber to cause said propagation velocity to vary along the length of said fiber.

3. The apparatus as defined in claim 2, wherein said fiber is tapered in discrete steps.

4. The apparatus as defined in claim 2, wherein said fiber is tapered gradually.

5. The apparatus as defined in claim 2, wherein said generator includes means for varying the frequency of said flexural wave.

6. The apparatus as defined in claim 5, wherein the taper of said fiber is selected such that the region over which substantial coupling occurs is small compared to the length of said fiber, the location of said region varying along said fiber as the frequency of said flexural wave is varied.

7. The apparatus as defined in claim 6, wherein the length of said fiber is at least about an order of magnitude greater than said coupling region.

8. The apparatus as defined in claim 6, wherein the length of said coupling region is on the order of a few beat lengths.

9. The apparatus as defined in claim 2, wherein said optical fiber comprises at least first and second portions, said first portion having a larger outer diameter than said second portion, said flexural wave in said first portion having a wavelength determined by a first frequency and a first propagation velocity, said second portion size to cause a flexural wave at a seCon frequency and at a second propagation velocity to have the same wavelength.

10. The apparatus as defined in claim 9, wherein the length of said first portion is selected to provide substantially complete coupling of light from one of said first and second propagation modes to the other of said first and second propagation modes at a first frequency of said flexural wave and the length of said second portion is selected to provide substantially complete coupling of light from one of said first and second propagation modes to the other of said first and second propagation modes at a second frequency of said flexural wave.

11. The apparatus as defined in claim 9, wherein:

said fiber includes a third portion having a diameter larger than the diameter of said first and second portions of said optical fiber; and

said diameter of said third portion being sized so that virtually no coupling between said first and second optical propagation modes occurs in said third portion of the fiber.

12. The apparatus as defined in claim 11, wherein said generator of said flexural wave is coupled to said optical fiber at said third portion of said optical fiber.

13. The apparatus as defined in claim 2, wherein said optical fiber comprises at least first and second portions, said first portion having a larger outer diameter than said second portion, said flexural wave having a first propagation velocity and a corresponding first flexural wavelength in said first portion and having a second propagation velocity and a corresponding second flexural wavelength in said second portion, said first flexural wavelength substantially equal to a first fiber beat length for light at a first optical frequency and said second flexural wavelength substantially equal to a second fiber beat length for light at a second optical frequency.

14. The apparatus as defined in claim 1, wherein said flexural wave comprises a mode of the first order group of flexural waves and forms a series of traveling microbends in said optical fiber.

15. The apparatus as defined in claim 14, wherein said optical fiber is a multimode optical fiber.

16. The apparatus as defined in claim 15, further including a mode selector comprising a second dissimilar optical fiber positioned in the evanescent field of said multimode optical fiber so that light propagating in said optical fiber in said second propagation mode is exclusively coupled to said second dissimilar optical fiber in a selected propagation mode of said second dissimilar optical fiber to thereby separate light propagating in said second propagation mode from light propagating in said first propagation mode.

17. The apparatus as defined in claim 15, wherein said multimode optical fiber comprises a core having a noncircular cross section.

18. The apparatus as defined in claim 17, wherein said fiber has a core of elliptical cross section, and wherein one of said modes includes two orthogonal lobe orientations, the degree of ellipticity of said core selected to cause said orthogonal lobe orientations to be non-degenerate.

19. The apparatus as defined in claim 1, wherein said flexural wave is a second order flexural wave which spatially displaces said fiber so as to apply a periodic lateral squeezing force to said fiber.

20. The apparatus as defined in claim 19, wherein said optical fiber is a birefringent single mode fiber having two orthogonal polarization modes.

21. The apparatus as defined in claim 20, wherein the orientation of said squeezing force is at an angle of substantially 45°

with respect to the axes of birefringence of said fiber.

22. The apparatus as defined in claim 1, wherein the efficiency of said coupling between said propagation modes in said fiber is dependent upon the cross-sectional dimensions of said fiber.

23. The apparatus as defined in claim 1, wherein the range of frequencies in which coupling occurs is dependent upon the cross-sectional dimensions of the fiber.

24. The apparatus as defined in claim 1, wherein the range of frequencies in which coupling occurs is dependent upon the frequency of said flexural wave.

25. The apparatus as defined in claim 1, wherein said wavelength of said flexural wave is selected to be substantially equal to the beat length of said fiber for light propagating therein.

26. The apparatus as defined in claim 1, wherein said first and second propagation modes have first and second optical propagation constants, respectively, for light propagating therein, and said flexural wave has a propagation constant which is substantially equal to the difference between said first and second optical propagation constants, such that said light is cumulatively coupled from one mode to the other.

27. The apparatus as defined in claim 1, wherein light traveling in said first propagation mode at a first optical frequency and a first phase propagation velocity is coupled to said second propagation mode at a second optical frequency and a second propagation velocity so that said second frequency is a sideband of said first optical frequency.

28. The apparatus as defined in claim 27, wherein said second optical frequency is equal to said first optical frequency plus said frequency of said flexural wave when the light in said fiber propagates in the same direction as said flexural wave and said first phase propagation velocity is greater than said second phase propagation velocity, and said second optical frequency is equal to said first optical frequency minus said frequency of said flexural wave when the light in said fiber propagates in the same direction as said flexural wave and said first phase velocity is less than said second phase velocity.

29. The apparatus as defined in claim 1, wherein said generator of said flexural wave comprises an acoustic transducer.

30. The apparatus as defined in claim 29, wherein said acoustic transducer produces longitudinal acoustic waves.

31. The apparatus as defined in claim 29, wherein said acoustic transducer produces torsional acoustic waves.

32. The apparatus as defined in claim 29, wherein said acoustic transducer produces flexural acoustic waves.

33. The apparatus as defined in claim 29, wherein said acoustic transducer comprises an elongated member having a first end mechanically coupled to said optical fiber and having a second end disposed away from said first end, said second end having a transducer disposed thereon, said transducer responsive to an electrical signal applied thereto to generate an acoustic wave which propagates from said second end of said member to said first end of said member to thereby induce said flexural waves in said optical fiber.

34. The apparatus as defined in claim 33, wherein said second end of said member is larger than said first end of said member so that the acoustic energy per unit area applied to said optical fiber is greater than the acoustic energy per unit area excited in said second end of said member by said transducer.

35. The apparatus as defined in claim 34, wherein said acoustic wave has a wavelength and said first end of said member has a cross-sectional dimension smaller than the wavelength of said acoustic wave.

36. The apparatus as defined in claim 34, wherein said transducer excites longitudinal mode acoustic waves in said member.

37. The apparatus as defined in claim 34, wherein said transducer excites surface acoustic waves at said second end, said member converting the energy of said surface waves to provide longitudinal waves at said first end of said member.

38. The apparatus as defined in claim 37, wherein said member comprises a cylinder which is hollow at said second end and is solid at said first end, the transition between said hollow end and said solid end being a smooth and gradual taper.

39. The apparatus as defined in claim 1, additionally comprising a damper, mechanically coupled to said optical fiber, to prevent reflection of said flexural wave traveling in said optical fiber.

40. The apparatus as defined in claim 1, wherein said optical fiber includes a portion in which the diameter of the cladding of said optical fiber decreases from a larger diameter to a smaller diameter, said generator coupled to said fiber at a location thereon at which the cladding diameter is sufficiently large to prevent coupling of light at said location.

41. The apparatus as defined in claim 1, wherein said coupling of light from one of said first and second modes to the other of said first an second moes occurs over a broad range of frequencies of said light propagating in said fiber.

42. An apparatus for coupling light, comprising:

an optical fiber having two propagation modes; and

an acoustic horn, acoustically coupled to said optical fiber and an acoustic transducer for generating surface acoustic waves on a surface of said horn, said horn configured to adiabatically transform said surface waves into longitudinal waves for exciting a flexural wave in said fiber to cause coupling of light between said modes.

43. The apparatus defined in claim 42 further comprising means for suppressing propagation of bulk acoustic waves in said horn.

44. An apparatus for coupling light between optical propagation modes in an optical fiber, comprising:

an optical fiber having a first optical propagation mode and a second optical propagation mode for light propagating therein, the cross-sectional dimensions of said fiber varying along the length of said fiber; and

a generator for producing an acoustic wave which propagates in said optical fiber, the energy of said traveling acoustic wave confined to said optical fiber, said acoustic wave having an acoustic frequency, said acoustic wave having a propagation velocity which varies with said varying cross-sectional imensions of said fiber and having a wavelength determined by said acoustic frequency and said propagation velocity, said wavelength of said acoustic wave selected to cause light to be coupled from one of said modes to the other of said modes.

45. An apparatus as defined by claim 44, wherein said cross-section of said fiber is gradually tapered.

46. An apparatus as defined by claim 45, wherein said cross-section of said fiber varies in discrete increments.

47. An apparatus for transforming low amplitude acoustic oscillations into high amplitude acoustic oscillations, comprising:

an acoustic medium having first and second ends, the cross-sectional area of said first end larger than the cross-sectional area of said second end; and

a transducer for producing surface acoustic waves in said first end which propagate to said second end, said medium having a transition region between said first and second ends, said transition region configured to substantially adiabatically transform said surface acoustic waves into longitudinal acoustic waves as said waves propagate from said first end to said second end.

48. The apparatus as defined in claim 47, wherein said medium further includes a cavity in said transition region for suppressing propagation of bulk acoustic waves in said medium.

49. The apparatus defined in claim 48, wherein said cavity is filled with a material which attenuates acoustic waves to suppress surface wave propagation within said cavity.

50. The apparatus as defined in claim 47, wherein said transducer comprises a piezoelectric material isposed on said first end of said medium, said piezoelectric material responsive to an electrical signal applied thereto to generate said surface acoustic waves.

51. The apparatus defined in claim 47, wherein the acoustic medium forms an acoustic horn for concentrating acoustic energy such that the acoustic energy per unit area applied to said first end is smaller than the acoustic energy per unit area at said second end.

52. The apparatus as defined in claim 47, wherein said second end has a cross-sectional dimension which is approximately equal to, or less than, the wavelength of the longitudinal mode acoustic waves.

53. A method of transforming surface acoustic waves into longitudinal acoustic waves comprising the steps of:

inducing a surface acoustic wave in a cylinder, said cylinder having first and second end portions with a transition portion therebetween, said first end portion having a larger diameter than said second end portion;

propagating said surface acoustic waves from said first end portion in the direction of said second end portion;

utilizing said transition portion to substantially adiabatically transform said surface acoustic waves into longitudinal mode acoustic waves; and

utilizing said transition portion to concentrate the energy of said surface acoustic waves such that the dominant acoustic wave mode at said second end of said cylinder is a longitudinal acoustic wave, having oscillations of higher amplitude than said oscillations of said surface acoustic wave induced at said first end portion.

54. The method defined in claim 53, further comprising the step of suppressing propagation of bulk acoustic waves in said transition portion.

55. A method of coupling light between optical propagation modes in an optical fiber comprising the steps of:

inputting light into an optical fiber having first and second optical propagation modes for light propagating therein; and

propagating a flexural wave in said optical fiber, said flexural wave having a frequency, propagation velocity and wavelength, said wavelength determined by said frequency and said propagation velocity, said wavelength selected so that a portion of said light propagating in one of said first and second propagation modes is coupled to the other of said first and and second propagation modes.

56. A method of coupling light between optical propagation modes in an optical fiber as defined in claim 55, further comprising the step of selecting the cross-sectional dimensions of said optical fiber such that the propagation velocity of said flexural wave varies along the length of said optical fiber.

57. A method of coupling light between optical propagation modes in an optical fiber as defined in claim 55, wherein said propagation step further comprises generating a series of traveling microbends in the fiber which propagate as a flexural wave of the first order group.

58. A method of coupling light between optical propagation modes in an optical fiber as defined in claim 57, further comprising the step of selecting said optical fiber such that said first and second optical propagation modes comprise first and second spatial modes of a multimode fiber.

59. A method of coupling light between optical propagation modes in an optical fiber as defined in claim 55, wherein said propagating step further comprises applying a periodic lateral squeezing force to said fiber to generate a second order flexural wave in said fiber.

60. A method of coupling light between optical propagation modes in an optical fiber as defined in claim 59, further comprising the step of selecting said optical fiber such that said first and second optical propagation modes comprise first and second polarization modes of a single-mode birefringent fiber.

61. A method of coupling light between optical propagation modes in an optical fiber as defined in claim 60, further comprising the step of applying said periodic squeezing force to said fiber at an angle with respect to the axes of birefringence of said fiber, said angle being about 45°

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