Optical articles for wavelength conversion and their manufacture and use

Claim 2

A process for wavelength conversion comprising the step of directing the incident optical waves for wavelength conversion through a series of aligned sections of optical materials for wavelength conversion, said sections being selected such that the sum for the series of sections of the product of the length of each section in the direction of alignment and the Δk for that section is equal to about zero, and such that the length of each section is less than its coherence length; wherein the Δk for each section is the difference between the sum of the propagation constants for the incident waves for the wavelength conversion system in that section and the sum of the propagation constant for the generated waves for the wavelength conversion system in that section, and the coherence length for each section is ##EQU16## for that section; and wherein either at least one of said materials is optically nonlinear or a layer of nonlinear optical material is provided adjacent to said series during wavelength conversion, or both.

Claim 3

A process for wavelength conversion in accordance with claim 1 wherein a Langmuir-Blodgett film is provided adjacent to said series during wavelength conversion.

Claim 4

The process for wavelength conversion in accordance with claim 1 wherein each section is constructed of nonlinear optical materials.

Claim 5

A process for wavelength conversion in accordance with claim 3 wherein incident waves of frequencies ω 1 and ω 2 are used to generate waves of frequency ω 3 ; and wherein ω 3 is equal to the sum of ω 1 and ω 2 .

Claim 6

A process for wavelength conversion in accordance with claim 3 wherein incident waves of frequency ω 4 is used to generate waves of frequencies ω 5 and ω 6 ; and wherein ω 4 is equal to the sum of ω 5 and ω 6 .

Claim 7

A process for wavelength conversion in accordance with claim 3 wherein second harmonic waves of the incident optical waves are generated.

Claim 8

A process for wavelength conversion in accordance with claim 3 wherein the aligned sections are pairs of adjacent sections of optical materials selected such that for each pair the sum of the product of the length of one section and its Δk together with the product of the length of the other section and its Δk is about zero.

Claim 9

A process for wavelength conversion in accordance with claim 7 wherein incident waves having a wavelength of 1.064 μm are used to generate second harmonic waves, and wherein the optical waves are directed through a waveguide having alternating sections of KTP and rubidium exchanged KTP.

Claim 10

A process for second harmonic generation in accordance with claim 8 wherein the waveguide width is about 6 μm, the length of each KTP section is about 1.3 μm and the length of each rubidium exchanged section is about 2.7 μm; and wherein the KTP is hydrothermally grown.

Claim 11

A process for wavelength conversion in accordance with claim 3 wherein the length of each section is in the range of 0.25 μm to 50 μm.

Claim 12

A process for wavelength conversion comprising the step of directing the incident optical waves for wavelength conversion through a wavelength conversion path having a series of aligned sections of optical materials for wavelength conversion; at least one of said optical materials having a Δk which is positive for said wavelength conversion; at least one of said optical materials having a Δk which is negative for said wavelength conversion; and the series of sections being selected such that the sum of the products of the lengths of each section of material having a positive Δk with its Δk is balanced with the sum of the products of the lengths of each section of material having a negative Δk with its Δk so that the overall coherence length over the wavelength conversion path is greater than the length of the wavelength conversion path.

Claim 13

A process for wavelength conversion comprising the step of directing the incident optical waves for wavelength conversion through a wavelength conversion path having a series of aligned sections of optical materials for wavelength conversion; at least one of said optical materials having a Δk which is positive for said wavelength conversion; at least one of said optical materials having a Δk which is negative for said wavelength conversion; and the series of sections being selected such that the sum of the products of the lengths of each section of material having a positive Δk with its Δk is balanced with the sum of the products of the lengths of each section of material having a negative Δk with its Δk so that the overall coherence length over the wavelength conversion path is greater than the length of the wavelength conversion path.

Claim 14

An optical article for use in a wavelength conversion system, said optical article comprising at least one optical conversion segment consisting of a series of aligned sections of optical materials for wavelength conversion, wherein said sections are selected so that the sum of the product of the length of each section and the Δk for that section is equal to about zero, and the length of each section is less than its coherence length; wherein the Δk for each section is the difference between the sum of the propagation constants for the incident waves for the wavelength conversion system in that section and the sum of the propagation constant for the generated waves for the wavelength conversion system in that section, and the coherence length for each section is ##EQU17## for that section; and wherein either at least one of said materials is optically nonlinear or said article thereby comprises a layer of nonlinear optical material adjacent to said segment, or both.

Claim 15

An optical article for use in a wavelength conversion system, said optical article comprising at least one optical conversion segment consisting of a series of aligned sections of optical materials for wavelength conversion, wherein said sections are selected so that the sum of the product of the length of each section and the Δk for that section is equal to about zero, and the length of each section is less than its coherence length; wherein the Δk for each section is the difference between the sum of the propagation constants for the incident waves for the wavelength conversion system in that section and the sum of the propagation constant for the generated waves for the wavelength conversion system in that section, and the coherence length for each section is ##EQU17## for that section; and wherein either at least one of said materials is optically nonlinear or said article thereby comprises a layer of nonlinear optical material adjacent to said segment, or both.

Claim 16

An optical article in accordance with claim 12 wherein a Langmuir-Blodgett film is provided adjacent to said segment.

Claim 17

The optical article in accordance with claim 12 wherein each section is constructed of nonlinear optical materials.

Claim 18

An optical article in accordance with claim 14 wherein the aligned sections are pairs of adjacent sections of optical materials selected such that for each pair the sum of the product of the length of one section and its Δk together with the product of the length of the other section and its Δk is about zero.

Claim 19

An optical article in accordance with claim 15 having alternating sections of KTP and rubidium exchanged KTP.

Claim 20

An optical article in accordance with claim 16 wherein said sections form a waveguide having a width of about 6 μm; wherein the length of each KTP section is about 1.3 μm and the length of each rubidium exchanged section is about 2.7 μm; and wherein the KTP is hydrothermally grown.

Claim 21

An optical article in accordance with claim 14 wherein the length of each section is in the range of 0.25 μm to 50 μm.

Claim 22

An optical article in accordance with claim 12 which is a waveguide comprising alternating sections of a crystalline substrate having the formula K 1-x Rb x TiOMO 4 wherein x is from zero to one and M is P or As, and sections of substrate material in which the cations of said substrate have been replaced by sufficient cations selected from the group consisting of Rb + , Cs + and Tl + to change the surface index of refraction with respect to the index of refraction of said substrate.

Claim 23

An optical article in accordance with claim 14 comprising alternating sections of single crystal KTiOPO 4 substrate and sections of substrate material in which the cations of said substrate are partially replaced by Rb.

Claim 24

An optical article in accordance with claim 14 comprising alternating sections of single crystal KTiOPO 4 substrate and sections of said substrate material wherein the cations are partially replaced by Tl + and Rb + .

Claim 25

An optical article in accordance with claim 12 wherein the optical materials are single crystal materials having the formula K 1-x Rb x TiOMO 4 wherein x is from 0 to 1 and M is selected from P and As, and single crystal materials of said formula where the cations have been replaced by at least one of Rb + , Tl + and Cs + .

Claim 26

An optical article in accordance with claim 22 which is a modified single crystal of KTiOPO 4 containing sections where the cations of KTiOPO 4 have been partially replaced by at least one of Rb + and Tl + .

Claim 27

In an optical waveguide device comprising at least one channel waveguide, means to couple an incoming optical wave into said channel waveguide and means to couple an outgoing wave out of said channel waveguide, the improvement wherein the channel waveguide is an optical article as provided in claim 12.

Claim 28

A process for preparing a channel waveguide for a wavelength conversion system comprising the steps of: (1) providing a z-cut substrate of crystalline material having the formula K 1-x Rb x TiOMO 4 wherein x is from zero to one and M is P or As or crystalline material having said formula wherein the cations have been partially replaced by Tl + , said substrate including an optically smooth surface with a selected portion at which it is suitable to form a channel waveguide; (2) providing a molten salt containing cations selected from the group consisting of Rb + , Cs + and Tl + in an amount efficient to provide upon exposure to said waveguide portion at a selected temperature for a selected time sufficient cation replacement to change the index of refraction with respect to the index of refraction of said substrate; (3) applying a masking material on said substrate to provide a pattern of aligned areas along said waveguide portion of said optically smooth surface which are alternately masked with a material resistant to said molten salt and unmasked; (4) immersing said masked substrate in said molten salt at said selected temperature for said selected time, thereby providing cation replacement in said unmasked areas; (5) removing the masking material from said substrate; and (6) finishing said substrate to provide a clean waveguide with polished waveguide input and output faces; the length of said masked and unmasked areas being selected such that after said cation replacement in the unmasked areas, a channel waveguide is provided at said portion which comprises at least one optical conversion segment consisting of a series of aligned sections of optical materials; and such that the sum for the series of sections of the product of the length of each section and the Δk for that section is equal to about zero, and the length of each section is less than its coherence length; wherein the Δk for each section is the difference between the sum of the propagation constants for the incident waves for the wavelength conversion system in that section and the sum of the propagation constant for the generated waves for said wavelength conversion system in that section, and the coherence length for each section is ##EQU18## for that section.

Claim 29

A process for preparing a channel waveguide for a wavelength conversion system comprising the steps of: (1) providing a z-cut substrate of crystalline material having the formula K 1-x Rb x TiOMO 4 wherein x is from zero to one and M is P or As or crystalline material having said formula wherein the cations have been partially replaced by Tl + , said substrate including an optically smooth surface with a selected portion at which it is suitable to form a channel waveguide; (2) providing a molten salt containing cations selected from the group consisting of Rb + , Cs + and Tl + in an amount efficient to provide upon exposure to said waveguide portion at a selected temperature for a selected time sufficient cation replacement to change the index of refraction with respect to the index of refraction of said substrate; (3) applying a masking material on said substrate to provide a pattern of aligned areas along said waveguide portion of said optically smooth surface which are alternately masked with a material resistant to said molten salt and unmasked; (4) immersing said masked substrate in said molten salt at said selected temperature for said selected time, thereby providing cation replacement in said unmasked areas; (5) removing the masking material from said substrate; and (6) finishing said substrate to provide a clean waveguide with polished waveguide input and output faces; the length of said masked and unmasked areas being selected such that after said cation replacement in the unmasked areas, a channel waveguide is provided at said portion which comprises at least one optical conversion segment consisting of a series of aligned sections of optical materials; and such that the sum for the series of sections of the product of the length of each section and the Δk for that section is equal to about zero, and the length of each section is less than its coherence length; wherein the Δk for each section is the difference between the sum of the propagation constants for the incident waves for the wavelength conversion system in that section and the sum of the propagation constant for the generated waves for said wavelength conversion system in that section, and the coherence length for each section is ##EQU18## for that section.

Claim 30

The process of claim 25 wherein the substrate of step (1) has the formula K 1-x Rb x TiOMO 4 .