Method for producing polarization inversion part, optical wavelength conversion element using the same, and optical waveguide

Claim 3

A method for manufacturing a polarization inversion part according to claim 1, wherein the treatment for reducing an internal electric field is at least one treatment selected from a heat treatment of the substrate at a temperature between 150° C. and a temperature less than the Curie temperature of the substrate and a treatment applying to the substrate a reverse direction electric field against the internal electric field.

Claim 4

A method for manufacturing a polarization inversion part according to claim 1, further comprising forming a polarization inversion stabilized part in an area near the surface of the substrate where polarization has been inverted at least once after reinverting the polarization.

Claim 5

A method for manufacturing a polarization inversion part according to claim 3, wherein the polarization inversion stabilized part is formed by a process comprising an ion exchange in the area.

Claim 6

A method for manufacturing a polarization inversion part according to claim 4, wherein the polarization inversion stabilized part is formed by a process comprising the ion exchange and a heat treatment at a temperature less than the Curie temperature of the substrate and not less than a temperature lower than the Curie temperature by 150° C., which is carried out after the ion exchange.

Claim 7

A method for manufacturing a polarization inversion part according to claim 1, comprising: forming a first electrode and a second electrode having a stripe pattern part on a surface or opposed surfaces of the substrate so that projection of the stripe pattern part of the one electrode in the polarization direction of the substrate fits into the stripe pattern part of the other electrode; developing the polarization inversion part from the first electrode side; and reinverting polarization in at least a part of the polarization inversion part from the second electrode side.

Claim 8

A method for manufacturing a polarization inversion part according to claim 1, comprising: forming a first electrode and a second electrode on a surface or opposed surfaces of the substrate, the second electrode having a stripe pattern part, the electrodes being formed so that projection of the stripe pattern part of the second electrode in the polarization direction of the substrate is included in the first electrode; developing the polarization inversion part from the first electrode side; and reinverting polarization in at least a part of the polarization inversion part from the second electrode side.

Claim 11

A method for manufacturing a polarization inversion part according to claim 8, wherein the polarization inversion stabilized part is formed by a process comprising an ion exchange of the polarization inversion part.

Claim 12

A method for manufacturing a polarization inversion part according to claim 9, wherein the polarization inversion stabilized part is formed by a process comprising the ion exchange and a heat treatment at a temperature lower than the Curie temperature of the substrate but not lower than the Curie temperature minus 150° C., which is carried out after the ion exchange.

Claim 13

A method for manufacturing a polarization inversion part according to claim 8, wherein the polarization part has a depth of 0.1 μm to 0.2 μm.

Claim 16

A method for manufacturing a polarization inversion part according to claim 12, wherein the second electric field element is larger than the first electric field element.

Claim 17

A method for manufacturing a polarization inversion part according to claim 12, wherein the second electric field element is 4 kV/mm or more and is lower than an electric field generating dielectric breakdown of the substrate.

Claim 18

A method for manufacturing a polarization inversion part according to claim 12, wherein the second electric field element is generated by a pulse voltage.

Claim 19

A method for manufacturing a polarization inversion part according to claim 15, wherein the first electric field element is generated by a pulse voltage whose pulse width is narrower than that of the pulse voltage generating the second electric field element.

Claim 20

A method for manufacturing a polarization inversion part according to claim 12, wherein the polarization direction and the surface of the substrate are substantially parallel.

Claim 21

A method for manufacturing a polarization inversion part according to claim 17, wherein a thickness of the substrate is 0.1 mm-0.4 mm.

Claim 22

A method for manufacturing a polarization inversion part according to claim 17, wherein the electric field is generated by a pair of electrodes arranged in the direction forming an angle of 2°-80° with the surface of the substrate.

Claim 23

A method for manufacturing a polarization inversion part according to claim 12, wherein the angle between the polarization direction and the surface is 1°-5°.

Claim 26

A method for manufacturing a polarization inversion part according to claim 21, wherein the low resistance part is formed by a process comprising an ion exchange.

Claim 27

A method for manufacturing a polarization inversion part according to claim 21, wherein two or more of the low resistance parts are substantially equally spaced between the first electrode and the second electrode.

Claim 28

A method for manufacturing a polarization inversion part according to claim 21, wherein the polarization direction and the surface are substantially parallel.

Claim 29

A method for manufacturing a polarization inversion part according to claim 21, wherein the angle between the polarization direction of the ferroelectric crystal and the surface is 1°-5°.

Claim 30

A method for manufacturing a polarization inversion part according to claim 25, wherein the low resistance part is formed with metal.

Claim 31

A method for manufacturing a polarization inversion part according to claim 26, wherein the low resistance part has a length of 10 μm-30 μm on the surface in the polarization direction.

Claim 32

A light wavelength conversion element comprising: a ferroelectric crystal substrate; a polarization inversion part formed within the substrate so as to form layers substantially parallel to each other; and a polarization inversion stabilized part formed within the polarization inversion part near the surface of the substrate, wherein the polarization inversion stabilized part is formed by a process including an ion exchange of the polarization inversion part, and has a depth of 0.01 μm to 0.2 μm.

Claim 33

A light wavelength conversion element comprising: a ferroelectric crystal substrate; a polarization inversion part formed within the substrate so as to form layers substantially parallel to each other; and a polarization inversion stabilized part formed within the polarization inversion part near the surface of the substrate, wherein the polarization inversion stabilized part is formed by a process including an ion exchange of the polarization inversion part, and has a depth of 0.01 μm to 0.2 μm.

Claim 34

A light wavelength conversion element comprising: a crystal having a nonlinear optical effect; an optical waveguide formed alone a surface in the crystal; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide and a thickness that is determined so that a fundamental wave propagating in the optical waveguide cannot propagate in the ion exchanged layer but a higher harmonic of the fundamental wave can propagate in the ion exchanged layer; and wherein the thickness of the ion exchanged layer corresponds to a diffraction limit of the higher harmonic or less.

Claim 35

A light wavelength conversion element comprising: a crystal having a nonlinear optical effect; an optical waveguide formed alone a surface in the crystal; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide and a thickness that is determined so that a fundamental wave propagating in the optical waveguide cannot propagate in the ion exchanged layer but a higher harmonic of the fundamental wave can propagate in the ion exchanged layer; and wherein the thickness of the ion exchanged layer corresponds to a diffraction limit of the higher harmonic or less.

Claim 36

A light wavelength conversion element according to claim 29, wherein a width of the ion exchanged layer is narrower than that of the optical waveguide.

Claim 37

A light wavelength conversion element according to claim 29, wherein the fundamental wave of a fundamental mode and the higher harmonic of a higher-order mode are in the state of phase matching within the optical waveguide.

Claim 38

A light wavelength conversion element according to claim 29, wherein the crystal is a ferroelectric crystal and the angle between the polarization direction of the crystal and the surface is 1°-5°.

Claim 39

A light wavelength conversion element according to claim 29, wherein a width of the ion exchanged layer is narrowed to a tapered end at an end of the optical waveguide.

Claim 40

A light wavelength conversion element comprising: a crystal having a nonlinear optical effect; an optical waveguide formed along a surface in the crystal; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; and an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide, a width narrower than that of the optical waveguide and a depth shallower than the half depth of the optical wave guide.

Claim 41

A light wavelength conversion element comprising: a crystal having a nonlinear optical effect; an optical waveguide formed along a surface in the crystal; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; and an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide, a width narrower than that of the optical waveguide and a depth shallower than the half depth of the optical wave guide.

Claim 42

A light generator comprising a light wavelength conversion element and a semiconductor laser, converting a wavelength of an outgoing beam from the semiconductor laser by the light wavelength conversion element, wherein the light wavelength conversion element comprises: a crystal having a nonlinear optical effect, an optical waveguide formed along a surface in the crystal; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide and a thickness that is determined so that a higher harmonic of a fundamental wave can propagate in the ion exchanged layer but for the fundamental wave propagating in the optical waveguide can not propagate in the ion exchanged layer; and wherein a fundamental mode of a fundamental wave of the beam is converted into a higher-order mode of a higher wave of the beam by the light wavelength conversion element, and at least a length in the diameter direction of a main peak of at least one sub-peak, other than the main peak having maximum intensity out of peaks in an intensity distribution of the higher-order mode of the higher harmonic wave, corresponds to the diffraction limit of the higher harmonic wave or less.

Claim 43

A light generator comprising a light wavelength conversion element and a semiconductor laser, converting a wavelength of an outgoing beam from the semiconductor laser by the light wavelength conversion element, wherein the light wavelength conversion element comprises: a crystal having a nonlinear optical effect, an optical waveguide formed along a surface in the crystal; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide and a thickness that is determined so that a higher harmonic of a fundamental wave can propagate in the ion exchanged layer but for the fundamental wave propagating in the optical waveguide can not propagate in the ion exchanged layer; and wherein a fundamental mode of a fundamental wave of the beam is converted into a higher-order mode of a higher wave of the beam by the light wavelength conversion element, and at least a length in the diameter direction of a main peak of at least one sub-peak, other than the main peak having maximum intensity out of peaks in an intensity distribution of the higher-order mode of the higher harmonic wave, corresponds to the diffraction limit of the higher harmonic wave or less.

Claim 44

An optical pick-up comprising a light generator, a focusing optical system and a recording medium, an outgoing beam from the light generator being focused on the recording medium by the focusing optical system, the light generator comprising a light wavelength conversion element and a semiconductor laser, converting a wavelength of an outgoing beam from the semiconductor laser by a light wavelength conversion element, wherein the light wavelength conversion element comprises; a crystal having a nonlinear optical effect; an optical waveguide formed along a surface in the crystal; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; and an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide and a thickness that is determined so that a higher harmonic of a fundamental wave can propagate in the ion exchanged layer but for the fundamental wave propagating in the optical waveguide can not propagate in the ion exchanged layer; and wherein a fundamental mode of a fundamental wave of the beam is converted into a higher-order mode of a higher wave of the beam by the light wavelength conversion element, and at least a length in the diameter direction of a main peak of at least one sub-peak, other than the main peak having maximum intensity out of peaks in an intensity distribution of the higher order mode of the higher harmonic wave, corresponds to the diffraction limit of the higher harmonic wave or less.

Claim 45

An optical pick-up comprising a light generator, a focusing optical system and a recording medium, an outgoing beam from the light generator being focused on the recording medium by the focusing optical system, the light generator comprising a light wavelength conversion element and a semiconductor laser, converting a wavelength of an outgoing beam from the semiconductor laser by a light wavelength conversion element, wherein the light wavelength conversion element comprises; a crystal having a nonlinear optical effect; an optical waveguide formed along a surface in the crystal; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; and an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide and a thickness that is determined so that a higher harmonic of a fundamental wave can propagate in the ion exchanged layer but for the fundamental wave propagating in the optical waveguide can not propagate in the ion exchanged layer; and wherein a fundamental mode of a fundamental wave of the beam is converted into a higher-order mode of a higher wave of the beam by the light wavelength conversion element, and at least a length in the diameter direction of a main peak of at least one sub-peak, other than the main peak having maximum intensity out of peaks in an intensity distribution of the higher order mode of the higher harmonic wave, corresponds to the diffraction limit of the higher harmonic wave or less.

Claim 46

An optical waveguide comprising: a crystal substrate; a waveguide formed along a surface in the crystal substrate; and an ion exchanged layer formed in a surface of the waveguide, wherein the ion exchanged layer has a refractive index larder than that of the waveguide and a thickness that is determined so that a higher harmonic of a fundamental wave can propagate in the ion exchanged layer but the fundamental wave propagating in the waveguide can not propagate in the ion exchanged layer; and wherein a thickness of the ion exchanged layer is a diffraction limit of the higher harmonic or less.

Claim 47

An optical waveguide comprising: a crystal substrate; a waveguide formed along a surface in the crystal substrate; and an ion exchanged layer formed in a surface of the waveguide, wherein the ion exchanged layer has a refractive index larder than that of the waveguide and a thickness that is determined so that a higher harmonic of a fundamental wave can propagate in the ion exchanged layer but the fundamental wave propagating in the waveguide can not propagate in the ion exchanged layer; and wherein a thickness of the ion exchanged layer is a diffraction limit of the higher harmonic or less.

Claim 48

An optical waveguide according to claim 37, wherein a width of the ion exchanged layer is narrower than that of the waveguide.

Claim 49

An optical waveguide according to claim 37, wherein the fundamental wave of a fundamental mode and the higher harmonic of a higher-order mode are in the state of phase matching within the waveguide.

Claim 50

An optical waveguide according to claim 37, wherein the angle between the polarization direction of the crystal and the surface is 1°-5°.

Claim 51

An optical waveguide according to claim 37, wherein a width of the layer having a high refractive index is narrowed to a tapered end at ends of the waveguide.

Claim 52

An optical waveguide comprising: a crystal substrate; a waveguide formed along a surface in the crystal substrate; and an ion exchanged layer formed in a surface of the waveguide, wherein the ion exchanged layer has a refractive index larger than that of the waveguide, a width narrower than that of the waveguide and a depth shallower than half the depth of the waveguide.

Claim 53

An optical waveguide comprising: a crystal substrate; a waveguide formed along a surface in the crystal substrate; and an ion exchanged layer formed in a surface of the waveguide, wherein the ion exchanged layer has a refractive index larger than that of the waveguide, a width narrower than that of the waveguide and a depth shallower than half the depth of the waveguide.

Claim 54

A light wavelength conversion element comprising: a substrate of a crystal with a nonlinear optical effect having an inclination angle of 1°-5° between a polarization direction and a surface of the substrate; an optical waveguide formed along a surface in the substrate; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; and an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide and a thickness thinner than the thickness between the upper end of the polarization inversion part and the substrate surface at the center of the width of the optical waveguide.

Claim 55

A light wavelength conversion element comprising: a substrate of a crystal with a nonlinear optical effect having an inclination angle of 1°-5° between a polarization direction and a surface of the substrate; an optical waveguide formed along a surface in the substrate; two or more polarization inversion parts formed so as to traverse the optical waveguide periodically; and an ion exchanged layer formed in a surface of the optical waveguide, wherein the ion exchanged layer has a refractive index larger than that of the optical waveguide and a thickness thinner than the thickness between the upper end of the polarization inversion part and the substrate surface at the center of the width of the optical waveguide.