IP Library Granted Patent US 11,269,236
Granted Patent B2
US 11,269,236 · App. 16/887,162 · Granted Mar 8, 2022

Tunable optical structures

Inventors: Erman Timurdogan (Somerville, MA); Ehsan Shah Hosseini (Boston, MA); Michael Robert Watts (Hingham, MA); Michael J. Whitson (Salem, MA)
Assignee: Analog Photonics LLC
G02F1/335G02F1/2955
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Quick Facts
Patent No.
US 11,269,236
App. No.
16/887,162
Granted
Mar 8, 2022
Kind
B2
Abstract

Aspects of the present disclosure describe optical structures and devices, and more particularly to improved, tunable optical structures including optical gratings that are dynamically affected and/or tuned by acousto-optic or electro-optic mechanisms.

Claims (32)

1. A method of forming an optical structure comprising:

providing an optical waveguide having a light guiding core;

inducing dynamic index perturbations in the light guiding core through an electro-optic effect, said dynamic index perturbations sufficient to affect the emission of light traversing the optical waveguide, said emission in a direction out-of-plane relative to the waveguide, where said direction is based at least in part on a spatial period of the dynamic index perturbations along the light guiding core;

wherein a plurality of contacts apply a voltage distribution along the waveguide, and the waveguide includes regions segmented into sections that are each controlled by an individual voltage applied by a respective one of the contacts.

2. The method of claim 1 , further comprising varying the induced dynamic index perturbations over time such that said direction changes over time in response to a change in the spatial period over time.

3. The method of claim 1 , wherein the core of the optical waveguide exhibits a thickness of less than 1λ, where λ is the wavelength of the light traversing the optical waveguide.

4. The method of claim 1 , wherein at least a portion of the out-of-plane emission of the light is in a perpendicular direction relative to a direction of travel of the traversing light.

5. The method of claim 1 , wherein said dynamic index perturbations are varied such that an emission angle associated with the out-of-plane emission varies with the varying dynamic index perturbations.

6. The method of claim 1 , wherein the optical structure is part of a phased array.

7. The method of claim 6 , wherein the phased array includes a plurality of emitters, each individual one of the emitters including an individual one of the optical structure.

8. The method of claim 7 , wherein each individual one of the optical structures includes an electro-optic transducer that upon activation induces the dynamic index perturbations into the waveguide, the electro-optic transducers operationally driven by an RF signal originating from a common source.

9. The method of claim 7 , wherein each individual one of the optical structures includes an electro-optic transducer that upon activation induces the dynamic index perturbations into the waveguide, the electro-optic transducers operationally driven by an individual RF signal originating from a respective individual source, each individual RF signal exhibiting a different frequency or phase offset from the other individual RF signals.

10. The method of claim 1 , wherein the spatial period corresponds to a period of a wave of an electrical signal along an electrode that applies an electric field across the light guiding core to induce the dynamic index perturbations.

11. The method of claim 10 , wherein the wave of the electrical signal comprises a standing wave.

12. The method of claim 10 , wherein the electrical signal comprises a radio frequency (RF) signal.

13. The method of claim 1 , wherein each section of a plurality of the sections includes a p-type doping region and an n-type doping region separated by an intrinsic region.

14. An optical device comprising:

an optical waveguide including a light guiding section;

a dynamic index perturbation generator configured to dynamically generate index perturbations in the light guiding section through an electro-optic effect;

such that upon activation of the dynamic index perturbation generator and the generation of index perturbations in the light guiding section, light traversing the light guiding section is emitted in a direction out-of-plane relative to the light guiding section, where said direction is based at least in part on a spatial period of the index perturbations along the light guiding section;

wherein the dynamic index perturbation generator includes a plurality of contacts configured to apply a voltage distribution along the waveguide, and the waveguide includes regions segmented into sections that are each controlled by an individual voltage applied by a respective one of the contacts.

15. The optical device of claim 14 , wherein the dynamic index perturbation generator is configured to vary the induced dynamic index perturbations over time such that said direction changes over time in response to a change in the spatial period over time.

16. The optical device of claim 14 , wherein the light guiding section exhibits a thickness of less than 1λ, where λ is the wavelength of the light traversing the optical waveguide.

17. The optical device of claim 14 , configured such that at least a portion of the out-of-plane emission of the light is in a perpendicular direction relative to a direction of travel of the traversing light.

18. The optical device of claim 14 , wherein the dynamic index perturbation generator is configured such that the dynamic index perturbations are varied and an emission angle associated with the out-of-plane emission varies with the varying dynamic index perturbations.

19. The optical device of claim 14 , wherein the optical device is part of a phased array that includes a plurality of emitters, each individual one of the emitters including an individual one of the optical device.

20. The optical device of claim 19 , wherein each individual one of the optical devices includes an electro-optic transducer that upon activation induces the dynamic index perturbations into the waveguide, the electro-optic transducers operationally driven by an RF signal originating from a common source.

21. The optical device of claim 19 , wherein each individual one of the optical devices includes an electro-optic transducer that upon activation induces the dynamic index perturbations into the waveguide, the electro-optic transducers operationally driven by an individual RF signal originating from a respective individual source, each individual RF signal exhibiting a different frequency or phase offset from the other individual RF signals.

22. The optical device of claim 14 , wherein the spatial period corresponds to a period of a wave of an electrical signal along an electrode of the dynamic index perturbation generator that applies an electric field across the light guiding section to generate the index perturbations.

23. The optical device of claim 22 , wherein wave of the electrical signal comprises a standing wave.

24. The optical device of claim 22 , wherein the electrical signal comprises a radio frequency (RF) signal.

25. The optical device of claim 14 , wherein each section of a plurality of the sections includes a p-type doping region and an n-type doping region separated by an intrinsic region.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jun 1, 2020
From: TIMURDOGAN, ERMAN; HOSSEINI, EHSAN; WATTS, MICHAEL; WHITSON, MICHAEL
To: ANALOG PHOTONICS LLC
Reel/Frame 052802/0114 →
Continuity (3)
Division 16132412 · Sep 15, 2018
Provisional Application 62558920 · Sep 15, 2017
Related Publication 20200292913A1 · Sep 17, 2020