Bi-domain two-mode single crystal fiber devices

• US 5,082,349 A
• Filed: 06/20/1990
• Issued: 01/21/1992
• Est. Priority Date: 04/25/1988
• 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: Cordova-Plaza, Amado, Shaw, Herbert J.
• Primary Examiner(s): ULLAH, AKM E
• Application Number:
  US07/541,091
• Time in Patent Office: 580 Days
• Field of Search: 350/96.15, 350/96.20, 350/96.29, 350/96.30, 350/96.31, 350/96.32, 350/96.33
• US Class Current: 385/2
• CPC Class Codes: G02F 1/0353 involving an electro-optic TE-TM mode conversion
• CPC Class Codes: G02F 1/3775 with a periodic structure, e.g. domain inversion, for quasi-phase-matching [QPM] G02F1/383 takes precedence

Abstract

A mode converter comprises an a-axis LiNbO₃ optical fiber exhibiting a ferroelectric bi-domain structure. The fiber is subject to an electrical field that induces a +π/2 phase retardation in one domain of the fiber and a -π/2 phase retardation in the other domain. A light signal launched in the fundamental mode of the fiber is converted into a light signal propagating in the second order mode. When the electrical field is selected so that the phase retardations are not multiples of π/2, the mode conversion is partial and the LiNbO₃ fiber can operate as an optical switch or as an amplitude modulator. The mode converter can also be operated as a second harmonic generator. The fiber is heated to a phase matching temperature so that a signal launched in the fundamental mode of the fiber and at a frequency ω is converted to the second order mode at a frequency 2ω. The LiNbO₃ fiber can also simultaneously operate as an optical switch and as a second harmonic generator. Other non-linear interactions are possible such as sum or difference frequency generation or parametric generation. The various embodiments of the present invention are reciprocal.

Claims

1. An apparatus, comprising:

an optical waveguide comprising a material having electro-optic properties, said optical waveguide including a first domain and a second domain, said domains collectively supporting a first optical propagation mode and a second optical propagation mode for optical energy propagating in said waveguide, said modes corresponding to first and second energy distribution patterns; and

a generator for producing a perturbation in the refractive index of one of said domains relative to the refractive index of the other of said domains of said optical waveguide, said perturbation altering the energy distribution of said optical energy to shift at least a portion of said optical energy from one of said patterns to the other of said patterns.

20. The apparatus as claimed in claim 1, wherein said perturbation produces heat, said single waveguide being heated to a phase matching temperature so that second harmonic generation occurs in said optical waveguide.

21. The apparatus as claimed in claim 1, wherein the optical energy input to said optical waveguide is at an input frequency ω

and the energy output from said optical waveguide is at a frequency twice the input frequency.

22. The apparatus as claimed in claim 21, wherein said perturbational generator also comprises an AC electrical source so that said apparatus operates as an optical switch.

23. The apparatus as claimed in claim 22, wherein the switch frequency of said apparatus is determined by said perturbational generator and is in the GHz range.

24. The apparatus as claimed in claim 22, wherein said second propagation mode has at least one lobe and said output waveguide is a single-mode waveguide sized so that the fundamental mode supported by said output waveguide matches the size of said at least one lobe of said second propagation mode.

25. The apparatus as claimed in claim 22, further comprising a multimode input waveguide for launching said optical signal into said signal crystal optical waveguide.

2. An apparatus, comprising:

a single crystal optical waveguide, said optical waveguide comprising lithium niobate, said optical waveguide providing first and second optical propagation modes for an optical signal propagating therein, said first and second optical propagation modes corresponding to first and second energy distribution patterns, said optical waveguide further comprising a bi-domain structure partitioning said optical waveguide in a first domain and in a second domain; and

a generator electrically perturbing the refractive index of said optical waveguide in said first domain relative to the refractive index of said second domain, said electrically induced perturbation being selected to cause a phase shift of light in said first domain relative to the light in said second domain so that at least a portion of the energy of said optical signal is transferred from one of said energy distribution patterns to the other.

3. The apparatus as claimed in claim 2, additionally comprising a second optical waveguide coupled to input light to said optical waveguide, said second optical waveguide being a single-mode optical waveguide.

4. The apparatus as claimed in claim 3, additionally comprising a third optical waveguide coupled to receive light from said optical waveguide, said third optical waveguide being a bimodal optical waveguide.

5. The apparatus as claimed in claim 4, wherein said second and third optical waveguides are polarization maintaining waveguides.

6. The apparatus as claimed in claim 2, wherein said perturbational generator comprises an electrical source for applying an electrical field within said single crystal waveguide.

7. The apparatus as claimed in claim 6, further comprising a plurality of electrodes for applying said electrical field to said single crystal waveguide.

8. The apparatus as claimed in claim 2, wherein said first and second domains are substantially of equal volume and are determined by the ferroelectric properties of the material of said single crystal optical waveguide.

9. The apparatus as claimed in claim 2, wherein said single crystal waveguide is an a-axis grown fiber.

10. The apparatus as claimed in claim 6, wherein said electric field produced by said electrical source induces a +π

/2 phase retardation in said first domain and a -π

/2 retardation in said second domain, so that the amplitudes of the energy distribution patterns in said first and second domains have opposite signs.

11. The apparatus as claimed in claim 2, wherein said first optical propagation mode corresponds to the fundamental mode and said second optical propagation mode corresponds to the second order mode.

12. The apparatus as claimed in claim 2, wherein said single crystal waveguide is oriented so as to use the largest electro-optic coefficient of lithium niobate.

13. The apparatus as claimed in claim 6, wherein said electric field produced by said electrical source induces phase retardations which are odd multiples of π

/2.

14. The apparatus as claimed in claim 2, additionally comprising an output waveguide for receiving light from said optical waveguide, said output waveguide being connected to one of said first and second domains, said perturbational generator alternatively changing the direction of the perturbation so that said apparatus functions as an optical switch.

15. The apparatus as claimed in claim 14, wherein said second propagation mode has at least one lobe and said output waveguide is a single-mode waveguide sized so that the fundamental mode supported by said output waveguide matches the size of said at least one lobe of said second propagation mode.

16. The apparatus as claimed in claim 14, further comprising a multimode input waveguide for launching said optical signal into said single crystal optical waveguide.

17. The apparatus as claimed in claim 14, wherein the switch frequency of said apparatus is determined by said perturbational source and is in the GHz range.

18. The apparatus as claimed in claim 6, wherein said electrical source induces phase retardations of ±

π

/4 for light in said first and second domains respectively.

19. The apparatus as claimed in claim 6, wherein said electrical source induces phase retardations selected such that said apparatus operates as an amplitude modulator.

26. The apparatus as claimed in claim 6, wherein said electrical field has a voltage given by the following equation:

##EQU36##

27. The apparatus as claimed in claim 6, wherein said single crystal waveguide is a crystal fiber and comprises a longitudinal axis, an a-axis and a c-axis orthogonal to each other, and wherein the longitudinal axis of said single crystal fiber is parallel to the a-axis of said single crystal fiber, the electrical field being collinear to the c-axis of said fiber.

28. A method of coupling optical energy in an optical waveguide, comprising the steps of:

providing a single crystal waveguide having electro-optic properties, said single crystal waveguide comprising a first and a second domain having first and second refractive indices, respectively, said waveguide including at least first and second spatial modes in said first and second domains, said first and said second refractive indices being equal when no perturbation is applied within said single crystal waveguide and changing differently upon applying a perturbation in said single crystal waveguide;

inputting a first optical signal having a first frequency into said single crystal waveguide, so that the first optical signal propagates in said first mode in said first domain and in said first mode in said second domain; and

perturbing the refractive index in said first and second domains to provide an output optical signal propagating at least in said second propagation mode.

29. A method of coupling optical energy in an optical waveguide as claimed in claim 28, wherein the step of perturbing the refractive index comprises the step of applying an electrical perturbation.

30. A method of coupling optical energy in an optical waveguide as claimed in claim 28, further comprising the step of inducing a +π

/2 phase retardation in said first domain and a -π

/2 retardation in said second domain, so that a total relative phase shift of π

is obtained between said first and second domains.

31. A method of coupling optical energy in an optical waveguide as claimed in claim 28, further comprising the steps of:

inducing a +π

/4 phase retardation in said first domain and a -π

/4 retardation in said second domain; and

alternately changing the direction of the electrical perturbation, so that conversion is partial between said first and second propagation modes, whereby the output optical signal varies in intensity between a maximum and a minimum corresponding to the alternation of the direction of the electrical perturbation.

32. A method of coupling optical energy in an optical waveguide as claimed in claim 28, further comprising the step of selecting phase retardations induced by said perturbation so as to modulate the amplitude of said output optical signal.

33. A method of coupling optical energy in an optical waveguide as claimed in claim 28, further comprising the step of heating said single crystal waveguide to a phase matching temperature so as to produce second harmonic generation in said single crystal waveguide.

34. A method of coupling optical energy in an optical waveguide as claimed in claim 28, further comprising the steps of:

inputting said first optical signal at an input frequency ω

into said single crystal waveguide in said first propagation mode; and

outputting said optical signal at a frequency twice the input frequency ω and

propagating in said second propagation mode.