Second-harmonic wave generating element

Claim 2

A second-harmonic wave generating element, comprising: a ferroelectric crystal substrate having an input portion for receiving an input wave having a fundamental frequency, an intermediate portion for converting said input wave to a wave having a frequency equal to the second harmonic of said fundamental frequency, and an output portion for emitting an output wave having a frequency equal to the second harmonic of said fundamental frequency, said intermediate portion being interposed between said input and output portions of said substrate; front-periodic and rear-periodic structures formed in the input and output portions of said substrate respectively, said periodic structures having alternating regions of high and low refractive indices along a surface of said substrate; and a second-harmonic wave generating structure formed in the intermediate portion of said substrate, whereby waves having a fundamental frequency entering said second-harmonic generating structure are confined between said front-periodic and rear-periodic structures.

Claim 3

The second-harmonic wave generating element according to claim 1, wherein the alternating regions of said front-periodic and rear-periodic structures include first portions of the high optical refractive index formed by the introduction of a material into said ferroelectric crystal substrate, said introduced material being different than that of the substrate; a period Λ i of the front-periodic structure has a value satisfying the following equation (1); a period Λ o of the rear-periodic structure has a value satisfying the following equation (2), ##EQU6## wherein, λ represents a wavelength of the fundamental wave in a vacuum; k 1 , k 2 , m 1 and m 2 , respectively represent zero or a positive integer; n(ω) represents a refractive index of the front-and rear-periodic structures with reference to the fundamental wave; and n(2ω) represents a refractive index of the periodic structures with reference to the second-harmonic wave.

Claim 4

The second-harmonic wave generating element according to claim 1, wherein the front-and rear-periodic structures comprise optical waveguides, respectively, each of the optical waveguides being provided with first alternating regions of the high optical refractive index formed by the introduction of a material different than that of said substrate to a first thickness d 1 into said ferroelectric crystal substrate and second alternating regions of the low optical refractive index formed by an introduction of the different kind of material to a second thickness d 2 into said ferroelectric crystal substrate where the first thickness d 1 is greater than the second thickness d 2 ; the period Λ i of the front-periodic structure has a value satisfying the following equation (A), and the period Λ o of the rear-periodic structure has a value satisfying the following equation (B), ##EQU7## wherein, λ is a wavelength of the fundamental wave in a vacuum; k 1 , k 2 , m 1 and m 2 , respectively are zero or a positive integer; n(ω)eff(d 1 ) is an effective refractive index, with reference to the fundamental wave, of the first alternating region of the first thickness d 1 ; n(ω)eff(d 2 ) is an effective refractive index, with reference to the fundamental wave, of the second alternating region of the second thickness d 2 ; n(2ω)eff(d 1 ) is an effective refractive index, with reference to the second-harmonic wave, of the first alternating region of the first thickness d 1 ; and n(2ω)eff(d 2 ) is an effective refractive index with reference to the second-harmonic wave of the second alternating region of the second thickness d 2 .

Claim 5

The second-harmonic wave generating element according to claim 1, wherein said second-harmonic wave generating structure has a nonlinear optical coefficient with a sign that is periodically reversed, and satisfies a quasi-phase-matching condition.

Claim 6

The second-harmonic wave generating element according to claim 2, wherein said second-harmonic wave generating structure has a nonlinear optical coefficient with a sign which is periodically reversed, satisfies a quasi-phase-matching condition.

Claim 7

The second-harmonic wave generating element according to claim 3, wherein said second-harmonic wave generating structure has a nonlinear optical coefficient with a sign which is periodically reversed, and satisfies a quasi-phase-matching condition.

Claim 8

A second-harmonic wave generating element comprising: a ferroelectric crystal substrate having a fundamental wave incident side and a wave emitting side; a second-harmonic wave generating means formed in a region of said substrate, for generating a second-harmonic wave of an incident fundamental wave; a front-periodic structure formed in a region of said substrate on the fundamental wave incident side and for receiving fundamental waves; a rear-periodic structure formed in a region of said substrate on the wave emitting side and for emitting generated second harmonic waves, said second-harmonic generating means being disposed between said front-periodic and rear-periodic structures; wherein the front-periodic structure and the rear-periodic structure each have first portions of a high optical refractive index and second portions of a low refractive index, said first and second portions of each structure being periodically and reciprocally arranged so that fundamental waves entering said second-harmonic generating means are confined between said front-periodic and rear-periodic structures.

Claim 9

A second-harmonic wave generating element comprising: a ferroelectric crystal substrate having a fundamental wave incident side and a wave emitting side; a second-harmonic wave generating means formed in a region of said substrate, for generating a second-harmonic wave of an incident fundamental wave; a front-periodic structure formed in a region of said substrate on the fundamental wave incident side and for receiving fundamental waves; a rear-periodic structure formed in a region of said substrate on the wave emitting side and for emitting generated second harmonic waves, said second-harmonic generating means being disposed between said front-periodic and rear-periodic structures; wherein the front-periodic structure and the rear-periodic structure each have first portions of a high optical refractive index and second portions of a low refractive index, said first and second portions of each structure being periodically and reciprocally arranged so that fundamental waves entering said second-harmonic generating means are confined between said front-periodic and rear-periodic structures.

Claim 10

A second-harmonic wave generating element according to claim 7, wherein said ferroelectric crystal substrate is a LiNbO 3 substrate, said first portions of the high optical refractive index comprise titanium diffused regions of said substrate, and said second portions comprise non-titanium diffused regions of said substrate.

Claim 11

A second-harmonic wave generating element according to claim 7, wherein said front-periodic and rear-periodic structures both have an optical waveguide extending along the wave propagating direction of said substrate and each optical waveguide is provided with said first and second portions of the respective periodic structure, the first and second portions being composed of a different kind of material than the substrate, the first and second portions being of two different thicknesses.

Claim 12

A second-harmonic wave generating element according to claim 8, wherein a periodic Λ i of the high and low optical refractive indices of the front-periodic structure has a value satisfying the following equation (1): ##EQU8## a period Λ o of the high and low refractive indices of the rear-periodic structure has a value satisfying the following equation (2): ##EQU9## wherein, λ represents a wavelength of the fundamental wave in a vacuum; k 1 , k 2 , m 1 and m 2 , respectively represent zero or a positive integer; n(ω) represents a refractive index of the front-and rear-periodic structures with reference to the fundamental wave; and n(2ω) represents a refractive index of the periodic structures with reference to the second-harmonic wave.

Claim 13

A second-harmonic wave generating element according to claim 9, wherein the period Λ i of the front-periodic structure has a value satisfying the following equation (A), and the period Λ o of the rear-periodic structure has a value satisfying the following equation (B), ##EQU10## wherein, λ is a wavelength of the fundamental wave in a vacuum; k 1 , k 2 , m 1 and m 2 , respectively are zero or a positive integer; n(ω)eff(d 1 ) is an effective refractive index, with reference to the fundamental wave, of the first portion of a first thickness d 1 ; n(ω)eff(d 2 ) is an effective refractive index, with reference to the fundamental wave, of the second portion of a second thickness d 2 ; n(2ω)eff(d 1 ) is an effective refractive index, with reference to the second-harmonic wave, of the first portion of the first thickness d 1 ; and n(2ω)eff(d 2 ) is an effective refractive index, with reference to the second-harmonic wave, of the second portion of the second thickness d 2 .

Claim 14

A second-harmonic wave generating element according to claim 7, wherein said second harmonic generating means has a nonlinear coefficient with a sign that is periodically reversed, and satisfies a quasi-phase-matching condition.

Claim 15

A second-harmonic wave generating element according to claim 10, wherein said second harmonic generating means has a nonlinear coefficient with a sign that is periodically reversed, and satisfies a quasi-phase-matching condition.

Claim 16

A second-harmonic wave generating element according to claim 11, wherein said second harmonic generating means has a nonlinear coefficient with a sign that is periodically reversed, and satisfies a quasi-phase-matching condition.