Fiber optic intermode coupling single sideband frequency shifter

• US 5,022,732 A
• Filed: 04/25/1989
• Issued: 06/11/1991
• Est. Priority Date: 01/17/1986
• 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: Engan, Helge E., Blake, James N., Shaw, Herbert J., Kim, Byoung Y.
• Primary Examiner(s): ULLAH, AKM E
• Application Number:
  US07/342,947
• Time in Patent Office: 777 Days
• Field of Search: 350/96.10, 350/96.15, 350/96.29, 350/96.30, 350/320, 350/358, 250/227
• US Class Current: 385/28
• 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. An acoustic wave is induced in a generator having a gradual tapered cross-section. The generator preferably has the shape of a horn and is coaxially mounted with said optical fiber, so as to suppress the acoustic wave induced in the optical fiber in the reverse direction.

Claims

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

an optical fiber having a longitudinal axis, said optical fiber supporting a first optical propagation mode and a second optical propagation mode for an optical signal 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 modes to the other of said modes, said generator of said flexural wave having a longitudinal axis substantially coaxial with the longitudinal axis of said optical fiber.

2. The apparatus as defined in claim 1, wherein said generator comprises a single transducer.

3. The apparatus as defined in claim 1, wherein said generator of said flexural wave comprises a plurality of transducers.

4. The apparatus as defined in claim 1, wherein said generator 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 being mounted around said optical fiber, said second end having at least one transducer distally disposed thereon, said transducer being 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 wave in said optical fiber.

5. The apparatus as defined in claim 4, 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.

6. The apparatus as defined in claim 4, wherein said transducer excites an acoustic wave at said second end, said member converting the energy of said acoustic wave to provide a flexural acoustic wave at said first end of said member.

7. The apparatus as defined in claim 4, 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.

8. The apparatus as defined in claim 4, wherein said member comprises damping material, said damping material surrounding said optical fiber and suppressing said flexural acoustic wave in a direction opposite the direction of propagation of said optical signal.

9. The apparatus as defined in claim 8, wherein said member is substantially collinear with said optical fiber, said member being mounted so that said member suppresses any acoustic wave propagating in said opposite direction.

10. The apparatus as defined in claim 4, further comprising a split block housing assembly, said housing assembly comprising a rear housing part and a front housing part, said rear housing part comprising an inner sleeve, said inner sleeve surrounded by the inner surface of said generator at said second end, said front housing part being removably mounted on said rear housing part.

11. The apparatus as defined in claim 10, wherein said generator and said fiber are supported coaxially by said split block housing assembly.

12. The apparatus as defined in claim 11, wherein said front housing part is bonded to said fiber by means of an adhesive.

13. The apparatus as defined in claim 4, wherein said member comprises two transducers distally mounted on said second end of said member.

14. The apparatus as defined in claim 13, wherein said distally mounted transducers are driven in opposition of phase by an electrical source.

15. The apparatus as defined in claim 2, wherein said transducer is driven by an AC electrical source.

16. The apparatus as defined in claim 3, wherein said plurality of transducers is driven by an electrical source at intervals selected so as to induce a flexural wave in said optical fiber.

17. The apparatus as defined in claim 4, wherein said member is formed from a single piece of material.

18. 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.

19. 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 being coupled to said fiber at a location thereon at which the cladding diameter is sufficiently large to prevent coupling of light at said location.

20. The apparatus as defined in claim 1, wherein said generator includes means for adiabatically transforming said acoustic waves so as to excite a flexural wave in said fiber, said flexural wave causing coupling of light between said modes.

21. The apparatus as defined in claim 1, wherein said cross-section of said fiber varies in discrete increments.

22. The apparatus as defined in claim 4, wherein said one transducer comprises a piece of piezoelectric material.

23. The apparatus as defined in claim 1, wherein said optical fiber is a multimode optical fiber or a birefringent single-mode fiber.

24. The apparatus as defined in claim 1, wherein said optical energy, traveling in said first propagation mode at a first optical frequency in 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 substantively equal to either the sum or difference of said first optical frequency and said frequency of said flexural wave.

25. The apparatus as defined in claim 24, wherein said second optical frequency is equal to said first optical frequency plus said frequency of said flexural wave when said optical signal 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 said optical signal propagates in the same direction as said flexural wave and said first phase velocity is less than said second phase velocity.

26. The apparatus as defined in claim 4, wherein said first end of said member is bonded to the circumference of said optical fiber with a low temperature melting glass having substantially a hardness similar to that of said optical fiber.

27. The apparatus as defined in claim 4, wherein said generator is made of a material such as glass, such that said first end of said generator may be slowly melted and fused to the circumference of said fiber.

28. The apparatus as defined in claim 3, wherein said transducers are separated from one another so as not to be electrically or mechanically connected together.

29. The apparatus as defined in claim 1, wherein said generator has the shape of a horn.

30. The apparatus as defined in claim 6, wherein said acoustic wave excited by said transducer at said second end is a surface acoustic wave.

31. A method of coupling optical energy between optical propagation modes in an optical fiber, comprising the steps of:

inputting an optical signal into an optical fiber having first and second optical propagation modes for signals propagating therein, said optical signal having a longitudinal axis;

propagating a flexural wave within said optical fiber, said flexural wave having a frequency, propagation velocity and wavelength within said fiber, said wavelength within said fiber being determined by said frequency and said propagation velocity, said wavelength being selected so that a portion of said optical energy propagating in one of said propagation modes is coupled to said other propagation mode; and

exciting said flexural wave by propagating acoustic energy in a direction substantially parallel to the longitudinal axis of said fiber.

32. The method as defined in claim 31, further comprising the step of suppressing propagation of said acoustic wave in said optical fiber in a direction opposite to the direction of propagation of said optical signal.

33. The method as defined in claim 31, wherein the step of inducing said acoustic wave comprises the step of inducing a surface acoustic wave.

34. A method of manufacturing a fiber optic frequency shifter comprising the steps of:

providing an optical fiber;

surrounding a portion of said optical fiber with an acoustic medium;

mounting and orienting acoustic transducers on said acoustic medium to generate an acoustic wave in said acoustic medium; and

driving said transducers on said acoustic medium so as to cause said acoustic wave to propagate in a direction substantially parallel to the longitudinal axis of said fiber, to thereby produce a flexural wave in said optical fiber.