Liquid crystal thermo-optic switch and element

• US 7,079,724 B2
• Filed: 11/24/2003
• Issued: 07/18/2006
• Est. Priority Date: 11/24/2003
• Status: Active Grant

• Current Assignee: John Ingalls Thackara
• Original Assignee: John Ingalls Thackara
• Inventors: Thackara, John Ingalls
• Primary Examiner(s): CONNELLY CUSHWA, MICHELLE R
• Application Number:
  US10/718,668
• Publication Number:
  US 20050111783A1
• Time in Patent Office: 967 Days
• Field of Search: 385 16- 24, 385/45
• US Class Current: 385/16
• CPC Class Codes: G02B 2006/12145 Switch
• CPC Class Codes: G02B 2006/1215 Splitter
• CPC Class Codes: G02B 6/266 the optical element being an attenuator
• CPC Class Codes: G02F 1/132 Thermal activation of liquid crystals exhibiting a thermo-optic effect
• CPC Class Codes: G02F 1/1326 Liquid crystal optical waveguides or liquid crystal cells specially adapted for gating or modulating between optical waveguides
• CPC Class Codes: G02F 1/3137 with intersecting or branching waveguides, e.g. X-switches and Y-junctions
• CPC Class Codes: G02F 2203/06 Polarisation independent
• CPC Class Codes: G02F 2203/48 Variable attenuator

Abstract

A channel waveguide switch, driven by liquid crystal thermo-optic elements, suitable for use in integrated optic applications. Two trenches, one on either side and parallel with the core region of a channel waveguide Y-branch, are filled with a liquid crystal material possessing positive birefringence. When a given trench is held at a temperature a few degrees below the clearing point, the liquid crystal is in its nematic phase with its director aligned along the long direction of the trench so that both polarizations of the guided mode are loaded by the liquid crystal'"'"'s ordinary refractive index. When the trench is held at a temperature a few degrees above the clearing point, both polarizations of the optical mode are loaded by the liquid crystal'"'"'s isotropic index. By holding the temperature of the second trench at the alternate temperature, the differential loading on the Y-branch causes the guided mode to be switched into the path loaded by the liquid crystal'"'"'s isotropic index. By controlling the liquid crystal temperature(s) at more than one location along the trench(s), the switch can be configured to operate as a variable attenuator.

Claims

1. An integrated optic switch comprising:

an optical Y-branch waveguide structure capable of guiding at least one optical mode and including;

a cladding medium;

a channel waveguide core disposed in said cladding medium and containing an input branch and first and second output branches;

a first elongated trench formed in said cladding medium and filled with a first liquid crystal material and laterally spaced apart from said channel waveguide core, the longitudinal axis of said first trench being disposed along one side of said input branch and said first output branch opposite to said second output branch;

said first liquid crystal material associated with the first output branch and having ordinary and isotropic refractive indices corresponding to nematic and isotropic phases of the first liquid crystal material, respectively; and

a first temperature control element disposed in heat exchange relationship with the first liquid crystal material, the first temperature control element being operative to selectively add heat to the first liquid crystal material to change the phase thereof from nematic to isotropic, thereby producing differential refractive index loading of the channel waveguide core such that at least a portion of optical mode light directed into one of the first and second output branches is redirected into the other of the first and second output branches.

2. The switch of claim 1, wherein the first liquid crystal material is positively birefringent.

3. The switch of claim 1, wherein the first liquid crystal material is negatively birefringent.

4. The switch of claim 1, further including a second elongated trench formed in said cladding medium and filled with a second liquid crystal material and laterally spaced apart from said channel waveguide core, the longitudinal axis of said second trench being disposed along a side of said input branch and said second output branch opposite to said first output branch, said second liquid crystal material being associated with the second output branch.

5. The switch of claim 4, wherein the second liquid crystal material possesses a fixed refractive index lying between the ordinary and isotropic refractive indices of the first liquid crystal material.

6. The switch of claim 5, wherein the first liquid crystal material is in the nematic phase possessing the ordinary refractive index at ambient temperatures.

7. The switch of claim 4, wherein the second liquid crystal material has ordinary and isotropic refractive indices that correspond to nematic and isotropic phases of the second liquid crystal material, respectively, the switch further including a second temperature control element disposed in heat exchange relationship with the second liquid crystal material and operative to selectively add heat to the second liquid crystal material, thereby changing the phase of the second liquid crystal from nematic to isotropic.

8. The switch of claim 1, wherein the cladding medium has a refractive index lying between the ordinary and isotropic indices of the first liquid crystal material.

9. The switch of claim 1, wherein the refractive index of the channel waveguide core is higher than the ordinary refractive index of the first liquid crystal material and higher than the isotropic refractive index of the first liquid crystal material.

10. The switch of claim 1, wherein one of or both the isotropic and ordinary refractive indices of the first liquid crystal material are higher than the refractive index of the channel waveguide core.

11. The switch of claim 10, wherein said first elongated trench has a cross-section which is smaller than a cross section of the channel waveguide core.

12. The switch of claim 11, wherein the first elongated trench has a substantially rectangular cross sectional shape and includes first and second sides, a top and a bottom, at least one of the first side, second side, top and bottom being provided with an alignment coating.

13. The switch of claim 1, wherein said first elongated trench has a first side, a second side, a top and a bottom, at least one of said first side, second side, top and bottom including an alignment coating.

14. The switch of claim 13, wherein the alignment coating comprises SiO and is deposited by oblique evaporation.

15. A variable optic attenuator comprising:

a cladding medium;

a channel waveguide core disposed in said cladding medium and capable of guiding at least one optical mode, the channel waveguide core containing at least one input branch and at least first and second output branches;

a first elongated trench formed in said cladding medium and filled with a first liquid crystal material and laterally spaced apart from said channel waveguide core, the longitudinal axis of said first trench being disposed along one side of said input branch and said first output branch opposite to said second output branch;

said first liquid crystal material associated with the first output branch and having ordinary and isotropic refractive indices corresponding to nematic and isotropic phases of the first liquid crystal material, respectively; and

one or more temperature control elements disposed in heat exchange relationship with the first liquid crystal material, each said temperature control element being operative to selectively add heat to a corresponding portion of the first liquid crystal material to change the phase thereof from nematic to isotropic, thereby producing differential refractive index loading of the channel waveguide core such that at least a portion of optical mode light directed into one of the first and second output branches is redirected into the other of the first and second output branches.

16. The variable optic attenuator of claim 15, wherein the first liquid crystal material is positively birefringent.

17. The variable optic attenuator of claim 15, wherein the first liquid crystal material is negatively birefringent.

18. The variable optic attenuator of claim 15, further including a second elongated trench formed in said cladding medium and filled with a second liquid crystal material and laterally spaced apart from said channel waveguide core, the longitudinal axis of said second trench being disposed alone a side of said input branch and said second output branch opposite to said first output branch, said second liquid crystal material being associated with the second output branch.

19. The variable optic attenuator of claim 18, wherein the second liquid crystal material possesses a fixed refractive index lying between the ordinary and isotropic refractive indices of the first liquid crystal material.

20. The variable optic attenuator of claim 19, wherein the first liquid crystal material is in the nematic phase possessing the ordinary refractive index at ambient temperatures.

21. The variable optic attenuator of claim 18, further including one or more temperature control elements disposed in heat exchange relationship with the second liquid crystal material and operative to selectively add heat to a corresponding portion of the second liquid crystal material to thereby change the phase thereof from nematic to isotropic.

22. The variable optic attenuator of claim 18, wherein each of said first and second trenches has a first side, a second side, a top and a bottom, at least one of said first side, second side, top and bottom including an alignment coating.

23. The variable optic attenuator of claim 22, wherein the alignment coatings comprise SiO deposited by oblique evaporation.

24. The variable optic attenuator of claim 15, wherein the cladding medium has a refractive index lying between the ordinary and isotropic indices of the first liquid crystal material.

25. The variable optic attenuator of claim 15, wherein the refractive index of the channel waveguide core is higher than the ordinary refractive index of the first liquid crystal material and higher than the isotropic refractive index of the first liquid crystal material.

26. The variable optic attenuator of claim 15, wherein one of or both the isotropic and ordinary refractive indices of the first liquid crystal material are higher than the refractive index of the channel waveguide core.

27. A liquid crystal thermo-optic element capable of being held in either of two polarization independent refractive index states, comprising:

a solid medium capable of transmitting optical radiation propagating along a given direction;

a liquid crystal material having ordinary and isotropic refractive indices corresponding, respectively, to nematic and isotropic phases, wherein, in the nematic phase, a first index of refraction is presented to optical radiation in the solid medium, and in the isotropic phase, a second index of refraction is presented to optical radiation in the solid medium and wherein said liquid crystal material is contained in at least one trench laterally spaced apart from said solid medium; and

a temperature control element disposed in heat exchange relationship with the liquid crystal material, the temperature control element being operative to selectively cause switching in the liquid crystal material between the nematic and isotropic phases to produce differential refractive index loading to said solid medium.

28. The liquid crystal thermo-optic element of claim 27, wherein the liquid crystal material is positively birefringent.

29. The liquid crystal thermo-optic element of claim 27, wherein the liquid crystal material is negatively birefringent.

30. The liquid crystal thermo-optic element of claim 27, wherein the trench has walls, at least one of which is coated with an alignment coating.

31. The liquid crystal thermo-optic element of claim 30, wherein the alignment coating comprises SiO.

32. The liquid crystal thermo-optic element of claim 31, wherein the alignment coating is provided by oblique evaporation.

33. A method for selectively directing light in an input branch of an optical structure into one or more of multiple output branches of the optical structure, at least one of said output branches being associated with a liquid crystal material that is contained in at least one trench laterally spaced apart from the input and output branches and that has ordinary and isotropic refractive indices corresponding, respectively, to nematic and isotropic phases, the liquid crystal material having a temperature control element in heat exchange relationship therewith, the method comprising:

launching light into the input branch of the optical structure; and

using the temperature control element to change the phase of the liquid crystal material from one to the other of the nematic and isotropic phases such that differential refractive index loading is generated to the input and output branches, thereby causing at least a portion of the light launched into the input branch of the optical structure to be redirected from one output branch into another.