In-guide control of optical propagation

• US 20030103708A1
• Filed: 09/10/2002
• Published: 06/05/2003
• Est. Priority Date: 11/30/2001
• Status: Active Grant

• Current Assignee: Photintech Inc.
• Original Assignee: Photintech Inc.
• Inventors: Zohrabyan, Armen, Galstian, Tigran, Birabassov, Rouslan, Tork, Amir, Dumont, Dany
• Granted Patent: US 6,859,567 B2
• Time in Patent Office: Days
• US Class Current: 385/1
• CPC Class Codes: G02F 1/0118 by controlling the evanescent coupling of light from a fibre into an active, e.g. electro-optic, overlay
• CPC Class Codes: G02F 1/1337 Surface-induced orientation of the liquid crystal molecules, e.g. by alignment layers
• CPC Class Codes: G02F 2202/022 polymeric
• CPC Class Codes: G02F 2203/055 wavelength filtering
• CPC Class Codes: G02F 2203/48 Variable attenuator

Abstract

We propose a dynamically tunable electro-optic cladding using our proprietary electro-optic material, applied to various circular and planar wave-guides along with specific electrode configuration and excitation electric field format appropriate to that material. Based on the evanescent field coupling phenomena, the proposed device may be used in variable optical attenuators, tunable filters and couplers, etc. Different design of applied electrodes and optical properties of controllable refractive index materials allow polarization dependent or independent, as well as direct or inverse operation regimes of proposed devices.

Claims

1. An optical device for controlling propagation of light within an optical waveguide comprising a core substantially axi-symmetrically surrounded by a cladding having a substantially fixed index of refraction, the optical device comprising:

a control region of the optical waveguide in which a radial thickness of the cladding is less than a penetration depth of an evanescent field of light propagating in the waveguide core;

a variable-index material surrounding the cladding at least within the control region, the variable-index material having an index of refraction that is controllable in response to an applied stimulus; and

a controller adapted to controllably apply the stimulus to the variable-index material within the control region.

2. An optical device as claimed in claim 1, wherein, at least within the control region of the optical waveguide, the thickness of the cladding is substantially uniform in a longitudinal direction of the waveguide.

3. An optical device as claimed in claim 1, wherein, at least within the control region of the optical waveguide, the thickness of the cladding varies with longitudinal position.

4. An optical device as claimed in claim 1, wherein the variable-index material comprises a liquid crystal material, and the stimulus comprises an electric field applied to the variable-index material substantially transversely to a longitudinal axis of the waveguide.

5. An optical device as claimed in claim 4, further comprising a surface treatment applied to an exterior surface of the cladding for defining a predetermined relaxed-state orientation of the liquid crystal in the absence of an electric field.

6. An optical device as claimed in claim 5, wherein the relaxed-state orientation comprises any one or more of:

a parallel orientation in which molecules of the liquid crystal lie substantially parallel to the longitudinal axis of the waveguide;

a radial orientation in which molecules of the liquid crystal lie substantially radially about the longitudinal axis of the waveguide;

a circumferential orientation in which molecules of the liquid crystal lie substantially circumferentially about the longitudinal axis of the waveguide; and

a helical orientation, in which molecules of the liquid crystal lie in a substantially helical path about the longitudinal axis of the waveguide.

7. An optical device as claimed in claim 5, wherein the relaxed-state orientation is the same throughout the control portion.

8. An optical device as claimed in claim 5, wherein the relaxed-state orientation is different at respective different longitudinal positions within the control portion.

9. An optical device as claimed in claim 4, wherein the controller comprises at least two electrodes disposed substantially symmetrically about the waveguide and defining a predetermined energized-state orientation of the liquid crystal in accordance with an electric field between the electrodes, the energized-state orientation of the liquid crystal being at least partially transverse to the core of the waveguide.

10. An optical device as claimed in claim 9, wherein the at least two electrodes comprises a first pair of electrodes disposed on opposite sides of the waveguide core.

11. An optical device as claimed in claim 10, wherein the at least two electrodes comprises a second pair of electrodes disposed on opposite sides of the waveguide core, the second pair of electrodes being controllable independently of the first pair of electrodes, and being angularly separated from the first pair of electrodes.

12. An optical device as claimed in claim 9, wherein the electrodes are oriented substantially parallel to the core.

13. An optical device as claimed in claim 9, wherein the electrodes are oriented at an angle to the core.

14. An optical device as claimed in claim 9, wherein a length of the electrodes substantially corresponds with the length of the control portion.

15. An optical device as claimed in claim 14, wherein each electrode is electrically contiguous, such that a substantially uniform electric field is generated within the control portion.

16. An optical device as claimed in claim 14, wherein each electrode is divided into a plurality of independently controllable electrode elements, such that a varying electric field can be generated within the control portion.

17. An optical device as claimed in claim 1, wherein the variable-index material is a solid-state material.

18. An optical device as claimed in claim 17, wherein the solid-state material is a birefringent material having a principle axis.

19. An optical device as claimed in claim 18, wherein the birefringent material is divided into at least one axial segment within the control portion, the principle axis of the birefringent material of each segment being arranged in a selected one of a plurality of orientations relative to the longitudinal axis of the waveguide.

20. An optical device as claimed in claim 19, wherein the plurality of orientations comprises:

a parallel orientation in which the principle axis lies substantially parallel to the longitudinal axis;

transverse orientation in which the principle axis lies substantially transverse to the longitudinal axis;

angled orientation in which the principle axis lies at an angle relative to the longitudinal axis; and

a helical orientation in which the principle axis follows a substantially helical path about the longitudinal axis.

21. An optical device as claimed in claim 19, wherein the selected orientation of the principle axis of the birefringent material is the same in each segment.

22. An optical device as claimed in claim 19, wherein the selected orientation of the principle axis of the birefringent material in one segment is different from that of at least one other segment.