Electro-optical sensor for detecting electric fields

Claim 2

An integrated optical waveguide device comprising a plurality of waveguide channels defined on a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other.

Claim 3

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein t he interferometer has no metallic components.

Claim 4

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein t he interferometer has no metallic components.

Claim 5

The interferometer of claim 2 wherein the interferometer comprises an electric field sensor.

Claim 6

The interferometer of claim 2 wherein the waveguide channels are adapted to receive a divided optical signal.

Claim 7

The interferometer of claim 2 wherein the interferometer comprises a voltage sensor.

Claim 8

The interferometer of claim 2 wherein the interferometer comprises an electro-optical signal modulator.

Claim 9

The interferometer of claim 2 wherein the interferometer comprises an electro-optical antenna capable of sensing electric fields.

Claim 10

The Mach-Zehnder interferometer of claim 2 wherein the reverse polarity of the waveguide channels is achieved by a method selected from the group consisting of titanium diffusion of at least one channel below T c of the waveguide material in the absence of an electric field, followed by proton exchange; titanium diffusion of at least one channel above T c of the waveguide material in the presence of an electric field followed by proton exchange; titanium diffusion of an interferometer below the temperature for domain inversion of the waveguide material followed by a temperature gradient effect induced by laser heating a channel and without subsequent proton exchange treatment; selective electron beam bombardment of at least one but less than all of the waveguide channels; titanium diffusion of both legs at a temperature above the T c of the waveguide material, each in the presence of a separate electric field, wherein said electric fields are opposite polarities and followed by either proton exchange treatment or titanium diffusion at a temperature below domain inversion; proton exchange and annealing below the T c of at least one but less than all of the waveguide channels; laser and non-laser temperature gradient effect of at least one but less than all of the waveguide channels; and ionic concentration gradient effect of at least one but less than all of the waveguide channels.

Claim 11

The Mach-Zehnder interferometer of claim 2 wherein the crystal material is lithium niobate.

Claim 12

The Mach-Zehnder interferometer of claim 2 wherein the crystal material is lithium tantalate.

Claim 13

An electric field sensor comprising an integrated optical waveguide device comprising a plurality of waveguide channels on a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, wherein one of said waveguide channels has titanium diffused therein, said diffusion being at a temperature below the Curie temperature of the crystal material followed by proton exchange treatment of the waveguide channels.

Claim 14

An electric field sensor comprising an integrated optical waveguide device comprising a plurality of waveguide channels on a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, wherein one of said waveguide channels has titanium diffused therein, said diffusion being at a temperature below the Curie temperature of the crystal material followed by proton exchange treatment of the waveguide channels.

Claim 15

The electric field sensor of claim 11 wherein the crystal material is lithium niobate.

Claim 16

The electric field sensor of claim 11 wherein at least one but less than all of the waveguide channels is exposed to selective electron beam bombardment.

Claim 17

The electric field sensor of claim 11 wherein the reverse polarity of the waveguide channels is achieved by laser irradiation of at least one but less than all of the waveguide channels.

Claim 18

The electric field sensor of claim 11 wherein the reverse polarity of the waveguide channels is achieved by a method selected from the group consisting of titanium diffusion of at least one channel below T c of the waveguide material in the absence of an electric field, followed by proton exchange; titanium diffusion of at least one channel above T c of the waveguide material in the presence of an electric field followed by proton exchange; titanium diffusion of an interferometer below the temperature for domain inversion of the waveguide material followed by a temperature gradient effect induced by laser heating a channel and without subsequent proton exchange treatment; selective electron beam bombardment of at least one but less than all of the waveguide channels; titanium diffusion of both legs at a temperature above the T c of the waveguide material, each in the presence of a separate electric field, wherein said electric fields are opposite polarities and followed by either proton exchange treatment or titanium diffusion at a temperature below domain inversion; proton exchange and annealing below the T c of at least one but less than all of the waveguide channels; laser and non-laser temperature gradient effect of at least one but less than all of the waveguide channels; and ionic concentration gradient effect of at least one but less than all of the waveguide channels.

Claim 19

The electric field sensor of claim 11 wherein the waveguide channels are parallel to each other.

Claim 20

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein the reverse polarity is achieved by titanium diffusion into at least one but less than all of said waveguide channels.

Claim 21

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein the reverse polarity is achieved by titanium diffusion into at least one but less than all of said waveguide channels.

Claim 22

The Mach-Zehnder interferometer of claim 17 wherein the reverse polarity is achieved in the absence of an electric field.

Claim 23

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein the crystal material is potassium titanyl phosphate.

Claim 24

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein the crystal material is potassium titanyl phosphate.

Claim 25

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein one of said waveguide channels has titanium diffused therein, wherein the titanium diffuses in the waveguide material to a depth greater than 0.10 microns.

Claim 26

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein one of said waveguide channels has titanium diffused therein, wherein the titanium diffuses in the waveguide material to a depth greater than 0.10 microns.

Claim 27

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein two of the waveguide channels possess an optical length difference relative to each other sufficient to produce quadrature phase bias.

Claim 28

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein two of the waveguide channels possess an optical length difference relative to each other sufficient to produce quadrature phase bias.

Claim 29

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein two of the waveguide channels possess an optical length difference relative to each other sufficient to produce π radian phase bias.

Claim 30

An electrode-less Mach-Zehnder interferometer comprising a plurality of waveguide channels defined in a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein the interferometer has no metallic components, and wherein two of the waveguide channels possess an optical length difference relative to each other sufficient to produce π radian phase bias.

Claim 31

An interferometer comprising: at least two parallel lithium niobate crystal waveguide channels, wherein at least one but less than all of the channels has been titanium diffused for such duration sufficient to diffuse titanium into said channel at a depth of at least 0.10 microns, whereby the titanium-diffused waveguide channel is caused to be reverse poled relative to its initial polarity, and wherein the waveguide channels have been proton exchanged by means of exposure to acid sufficient to replace at least some of the lithium ions in the waveguide channels with hydrogen ions.

Claim 32

An interferometer comprising: at least two parallel lithium niobate crystal waveguide channels, wherein at least one but less than all of the channels has been titanium diffused for such duration sufficient to diffuse titanium into said channel at a depth of at least 0.10 microns, whereby the titanium-diffused waveguide channel is caused to be reverse poled relative to its initial polarity, and wherein the waveguide channels have been proton exchanged by means of exposure to acid sufficient to replace at least some of the lithium ions in the waveguide channels with hydrogen ions.

Claim 33

An improved method of modulating an optical signal when a voltage potential is applied to an electro-optic crystal, said method comprising the steps: (a) exposing to a voltage potential a Mach-Zehnder interferometer comprising an electro-optic crystal in which at least one but less than all of the waveguide channels thereon has been reverse poled; (b) introducing an optical input signal to the Mach-Zehnder interferometer, whereby the optical signal is modulated within the Mach-Zehnder interferometer by the voltage potential.

Claim 34

An improved method of modulating an optical signal when a voltage potential is applied to an electro-optic crystal, said method comprising the steps: (a) exposing to a voltage potential a Mach-Zehnder interferometer comprising an electro-optic crystal in which at least one but less than all of the waveguide channels thereon has been reverse poled; (b) introducing an optical input signal to the Mach-Zehnder interferometer, whereby the optical signal is modulated within the Mach-Zehnder interferometer by the voltage potential.

Claim 35

The method of claim 24 wherein the electro-optic crystal is lithium niobate.

Claim 36

An electrode-less optical interferometric modulator comprising: an input waveguide section; an input branching section for dividing an optical signal on said input section into two substantially equal portions; first and second branch waveguides for transmitting the two portions of the divided optical signal; an output branching section for combining the optical signals on said first and second branch waveguides to form an optical output signal; a means for applying an electric field to the branch waveguides in the modulator; characterized in that said first and second branch waveguides are of reverse polarity relative to each other, whereby the optical output signal is modulated at the same frequency as the electric field.

Claim 37

An electrode-less optical interferometric modulator comprising: an input waveguide section; an input branching section for dividing an optical signal on said input section into two substantially equal portions; first and second branch waveguides for transmitting the two portions of the divided optical signal; an output branching section for combining the optical signals on said first and second branch waveguides to form an optical output signal; a means for applying an electric field to the branch waveguides in the modulator; characterized in that said first and second branch waveguides are of reverse polarity relative to each other, whereby the optical output signal is modulated at the same frequency as the electric field.

Claim 38

The optical interferometric modulator of claim 26 further comprising a means for optically decoupling said first and second branch waveguides.

Claim 39

An electrode-less, non-metallic voltage sensor comprising a plurality of waveguide channels defined on a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other.

Claim 40

An electrode-less, non-metallic voltage sensor comprising a plurality of waveguide channels defined on a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other.

Claim 41

An electrode-less, non-metallic voltage sensor comprising a plurality of waveguide channels defined on a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein one of said waveguide channels has titanium diffused therein, said diffusion being at a temperature below the Curie temperature of the crystal material.

Claim 42

An electrode-less, non-metallic voltage sensor comprising a plurality of waveguide channels defined on a crystal material, wherein two of the waveguide channels have reverse polarity relative to each other, and wherein one of said waveguide channels has titanium diffused therein, said diffusion being at a temperature below the Curie temperature of the crystal material.

Claim 43

The voltage sensor of claim 29 wherein the crystal material is lithium niobate.