Optical wavelength converting device for converting fundamental waves into harmonic waves and shorter wavelength coherent light generating apparatus with the device

Claim 2

An optical wavelength converting device, comprising: a ferroelectric substrate having an upper surface of which a normal line is inclined to a C-crystal axis toward an X-Y crystalline plane defined as (001) crystalline plane in Miller indices, spontaneous polarization of the ferroelectric substrate being directed toward a +C-crystal axis direction of the C-crystal axis; a plurality of inverted-polarization layers arranged at regular intervals in an upper surface region of the ferroelectric substrate, polarization of the inverted-polarization layers being directed toward a -C-crystal axis direction of the C-crystal axis, and the inverted-polarization layers being formed by exchanging positive ions included in the ferroelectric substrate for H + ions; and an optical waveguide crossing alternate rows of the inverted-polarization layers and the ferroelectric substrate positioned between the inverted-polarization layers, a part of fundamental waves transmitting through the optical waveguide being convened into second harmonic waves, and a refractive index of the optical waveguide being higher than that of the ferroelectric substrate to confine the fundamental and second harmonic waves in the optical waveguide.

Claim 3

A device according to claim 1 in which the normal line of the upper surface of the ferroelectric substrate is inclined at an angle of 90 degrees to the C-crystal axis toward the X-Y crystalline plane, and an extending direction of each of the inverted-polarization layers is inclined at an angle of six degrees or more to the C-crystal axis.

Claim 4

A device according to claim 2 in which the extending direction of each of the inverted-polarization layers is inclined at an angle ranging from 6 degrees to 174 degrees to the C-crystal axis, and the optical waveguide extends in a coherent light transmitting direction perpendicular to the C-crystal axis.

Claim 5

A device according to claim 1 in which a rising direction of the normal line of the upper surface of the ferroelectric substrate is inclined at an angle ranging from 60 degrees to 85 degrees to a -C-crystal axis direction.

Claim 6

A device according to claim 4 in which an extending direction of each of the inverted-polarization layers is reclined at an angle ranging from 6 degrees to 174 degrees to an X-C crystalline plane defined as (010) crystalline plane in the Miller indices, and the optical waveguide extends in a coherent light transmitting direction perpendicular to the C-crystal axis.

Claim 7

A device according to claim 4 in which an extending direction of each of the inverted-polarization layers is parallel to an X-C crystalline plane defined as (010) crystalline plane in the Miller indices, and the optical waveguide extends in a coherent light transmitting direction perpendicular to the C-crystal axis.

Claim 8

A device according to claim 1 in which a difference in a refractive index between the inverted-polarization layers and the ferroelectric substrate positioned in the optical waveguide is 0.005 or less to prevent a transmission loss of the fundamental and second harmonic waves transmitting through the optical waveguide from being increased.

Claim 9

A device according to claim 1 in which a width of each of the inverted-polarization layers ranges from 1 μm to 10 μm.

Claim 10

A device according to claim 1 in which the regular intervals of the inverted-polarization layers are respectively set to an equal distance ranging from 3 μm to 5 μm to obtain blue light consisting of the second harmonic waves on condition that a quasi-phase-matching condition Λ=λ f/ {2*(N2ω-Nω)} is satisfied, where the symbol Λ denotes the regular intervals, the symbol λ f denotes a wavelength of the fundamental waves, the symbol N2ω denotes an effective refractive index of the optical waveguide for the second harmonic waves, and the symbol Nω denotes an effective refractive index of the optical waveguide for the fundamental waves.

Claim 11

A device according to claim 1 in which the ferroelectric substrate is made of ferroelectric substance selected from the group consisting of: pure LiTaO 3 crystal; LiTaO 3 crystal doped by any of MgO, Nb, or Nd; pure LiNbO 3 crystal; and LiNbO 3 crystal doped by any of MgO, Ta, or Nd.

Claim 12

A device according to claim 1 in which each of the inverted-polarization layers is formed in a stripe shape.

Claim 13

A device according to claim 1, additionally including: a plurality of gratings periodically arranged on the optical waveguide at grating intervals in parallel to the inverted-polarization layers, a first refractive index of the gratings being equal to N1; and a covering layer arranged between the gratings to produce a periodic structure, a second refractive index of the covering layer being equal to N2 which differs from the first refractive index N1 of the gratings to form a diffraction grating in the periodic structure, and the fundamental waves which are not converted into the second harmonic waves being reflected by the diffraction grating.

Claim 14

A device according to claim 1, additionally including: a first electrode arranged on the ferroelectric substrate and the inverted-polarization layers positioned in the +C-crystal axis direction to the optical waveguide; a second electrode arranged on the ferroelectric substrate and the inverted-polarization layers positioned in the -C-crystal axis direction to the optical waveguide; and an electric source for applying an electric potential difference between the first and second electrodes, the electric field being induced through the optical waveguide between the first and second electrodes to change a first refractive index of the inverted-polarization layers in the optical waveguide and a second refractive index of the ferroelectric substrate in the optical waveguide, an increase or decrease of the first refractive index being opposite to that of the second refractive index to produce a diffraction grating formed of periodic change of the first and second refractive indexes in the optical waveguide, and the fundamental waves which are not converted into the second harmonic waves being reflected by the diffraction grating.

Claim 15

A device according to claim 1, additionally including: a plurality of second invented-polarization layers arranged in parallel to the inverted-polarization layers at second regular intervals to cross the optical waveguide, polarization of the second inverted-polarization layers being directed toward the -C-crystal axis direction, and the second inverted-polarization layers being formed by exchanging positive ions included in the ferroelectric substrate for H + ions; and a first electrode arranged on the ferroelectric substrate and the second inverted-polarization layers positioned in the +C-crystal axis direction to the optical waveguide; a second electrode arranged on the ferroelectric substrate and the second inverted-polarization layers positioned in the -C-crystal axis direction to the optical waveguide; and an electric source for applying an electric potential difference between the first and second electrodes, the electric field being induced through the optical waveguide between the first and second electrodes to change a first refractive index of the second inverted-polarization layers in the optical waveguide and a second refractive index of the ferroelectric substrate in the optical waveguide, an increase or decrease of the first refractive index being opposite to that of the second refractive index to produce a diffraction grating formed of periodic change of the first and second refractive indexes in the optical waveguide, and the fundamental waves which are not converted into the second harmonic waves being reflected by the diffraction grating.

Claim 16

A shorter wavelength coherent light generating apparatus, comprising: a semiconductor laser for radiating coherent light consisting of fundamental waves: and an optical wavelength convening device for converting the fundamental waves radiated from the semiconductor laser into second harmonic waves of which a wavelength is half of that of the fundamental waves, comprising a ferroelectric substrate having an upper surface of which a normal line is inclined to a C-crystal axis toward an X-Y crystalline plane defined as (001) crystalline plane in Miller indices, spontaneous polarization of the ferroelectric substrate being directed toward a +C-crystal axis direction of the C-crystal axis, a plurality of inverted-polarization layers arranged at regular intervals in an upper surface region of the ferroelectric substrate, polarization of the inverted-polarization layers being directed toward a -C-crystal axis direction of the C-crystal axis, and the inverted-polarization layers being formed by exchanging positive ions included in the ferroelectric substrate for H + ions, and an optical waveguide crossing alternate rows of the inverted-polarization layers and the ferroelectric substrate positioned between the inverted-polarization layers, a refractive index of the optical waveguide being higher than that of the ferroelectric substrate to confine the fundamental waves radiated from the semiconductor laser, and the fundamental waves being converted into second harmonic waves in the alternate rows of the optical waveguide.

Claim 17

A shorter wavelength coherent light generating apparatus, comprising: a semiconductor laser for radiating coherent light consisting of fundamental waves: and an optical wavelength convening device for converting the fundamental waves radiated from the semiconductor laser into second harmonic waves of which a wavelength is half of that of the fundamental waves, comprising a ferroelectric substrate having an upper surface of which a normal line is inclined to a C-crystal axis toward an X-Y crystalline plane defined as (001) crystalline plane in Miller indices, spontaneous polarization of the ferroelectric substrate being directed toward a +C-crystal axis direction of the C-crystal axis, a plurality of inverted-polarization layers arranged at regular intervals in an upper surface region of the ferroelectric substrate, polarization of the inverted-polarization layers being directed toward a -C-crystal axis direction of the C-crystal axis, and the inverted-polarization layers being formed by exchanging positive ions included in the ferroelectric substrate for H + ions, and an optical waveguide crossing alternate rows of the inverted-polarization layers and the ferroelectric substrate positioned between the inverted-polarization layers, a refractive index of the optical waveguide being higher than that of the ferroelectric substrate to confine the fundamental waves radiated from the semiconductor laser, and the fundamental waves being converted into second harmonic waves in the alternate rows of the optical waveguide.

Claim 18

An apparatus according to claim 15 in which the normal line of the upper surface of the ferroelectric substrate is inclined at an angle of 90 degrees to the C-crystal axis toward the X-Y crystalline plane, and an extending direction of each of the inverted-polarization layers is inclined at an angle of six degrees or more to the C-crystal axis.

Claim 19

An apparatus according to claim 16 in which the extending direction of each of the inverted-polarization layers is inclined at an angle ranging from 6 degrees to 174 degrees to the C-crystal axis, and the optical waveguide extends in a coherent light transmitting direction perpendicular to the C-crystal axis.

Claim 20

An apparatus according to claim 15 in which a rising direction of the normal line of the upper surface of the ferroelectric substrate is inclined at an angle ranging from 60 degrees to 85 degrees to a -C-crystal axis direction.

Claim 21

An apparatus according to claim 18 in which an extending direction of each of the inverted-polarization layers is inclined at an angle ranging from 6 degrees to 174 degrees to an X-C crystalline plane defined as (010) crystalline plane in the Miller indices, and the optical waveguide extends in a coherent light transmitting direction perpendicular to the C-crystal axis.

Claim 22

An apparatus according to claim 18 in which an extending direction of each of the inverted-polarization layers is parallel to an X-C crystalline plane defined as (010) crystalline plane in the Miller indices, and the optical waveguide extends in a coherent light transmitting direction perpendicular to the C-crystal axis.

Claim 23

An apparatus according to claim 15 in which a difference in a refractive index between the inverted-polarization layers and the ferroelectric substrate positioned in the optical waveguide is 0.005 or less to prevent a transmission loss of the fundamental and second harmonic waves transmitting through the optical waveguide from being increased.

Claim 24

An apparatus according to claim 15 in which a width of each of the inverted-polarization layers range from 1 μm to 10 μm.

Claim 25

An apparatus according to claim 15 in which the regular intervals of the inverted-polarization layers are respectively set to an equal distance ranging from 3 μm to 5 μm to obtain blue light consisting of the second harmonic waves on condition that a quasi-phase-matching condition Λ=λ f /{2*(N2ω-Nω)} is satisfied, where the symbol Λ denotes the regular intervals, the symbol λ f denotes a wavelength of the fundamental waves, the symbol N2ω denotes an effective refractive index of the optical waveguide for the second harmonic waves, and the symbol Nω denotes an effective refractive index of the optical waveguide for the fundamental waves.

Claim 26

An apparatus according to claim 15 in which the ferroelectric substrate is made of ferroelectric substance selected from the group consisting of: pure LiTaO 3 crystal; LiTaO 3 crystal doped by any of MgO, Nb, or Nd; pure LiNbO 3 crystal; and LiNbO 3 crystal doped by any of MgO, Ta, or Nd.

Claim 27

An apparatus according to claim 15 in which each of the inverted-polarization layers is formed in a stripe shape.

Claim 28

An apparatus according to claim 15, the optical wavelength converting device additionally including: a plurality of gratings periodically arranged on the optical waveguide at grating intervals in parallel to the inverted-polarization layers, a first refractive index of the gratings being equal to N1; and a covering layer arranged between the gratings to produce a periodic structure, a second refractive index of the covering layer being equal to N2 which differs from the first refractive index N1 of the gratings to form a diffraction grating in the periodic structure, the coherent light of a particular wavelength being selectively reflected by the diffraction grating, and the coherent light reflected being returned to the semiconductor laser to fix the wavelength of the coherent light radiated from the semiconductor laser to the particular wavelength.

Claim 29

An apparatus according to claim 15, the optical wavelength converting device additionally including: a first electrode arranged on the ferroelectric substrate and the inverted-polarization layers positioned in the +C-crystal axis direction to the optical waveguide; a second electrode arranged on the ferroelectric substrate and the inverted-polarization layers positioned in the -C-crystal axis direction to the optical waveguide; and an electric source for applying an electric potential difference between the first and second electrodes to induce electric field through the optical waveguide between the first and second electrodes, a first refractive index of the inverted-polarization layers in the optical waveguide and a second refractive index of the ferroelectric substrate in the optical waveguide being changed according to intensity of the electric field on condition that increase or decrease of the first refractive index is opposite to that of the second refractive index to produce a diffraction grating formed of alternate changes of the first and second refractive indexes in the optical waveguide, the coherent light of a particular wavelength being selectively reflected by the diffraction grating, and the coherent light reflected being returned to the semiconductor laser to fix the wavelength of the coherent light radiated from the semiconductor laser to the particular wavelength.

Claim 30

An apparatus according to claim 15 in which the semiconductor laser is directly attached to an incident end facet of the optical waveguide to transmit the coherent light polarized in a transverse electric mode through the optical waveguide.

Claim 31

An apparatus according to claim 15, additionally including an optical system for converging the coherent light radiated from the semiconductor laser at an incident end facet of the optical waveguide while maintaining the coherent light polarized in a transverse electric mode.

Claim 32

An apparatus according to claim 15, the optical wavelength converting device additionally including: a first electrode arranged on the ferroelectric substrate and the inverted-polarization layers positioned in the +C-crystal axis direction to the optical waveguide; a second electrode arranged on the ferroelectric substrate and the inverted-polarization layers positioned in the -C-crystal axis direction to the optical waveguide; and an electric source for periodically applying an electric potential difference between the first and second electrodes to periodically induce electric field through the optical waveguide between the first and second electrodes, a first refractive index of the inverted-polarization layers in the optical waveguide and a second refractive index of the ferroelectric substrate in the optical waveguide being periodically changed according to intensity of the electric field periodically induced on condition that increase or decrease of the first refractive index is opposite to that of the second refractive index to produce a diffraction grating formed of alternate changes of the first and second refractive indexes in the optical waveguide, the coherent light of a particular wavelength being selectively and periodically reflected by the diffraction grating, the coherent light reflected being returned to the semiconductor laser to fix the wavelength of the coherent light radiated from the semiconductor laser to the particular wavelength, and the second fundamental waves of a second particular wavelength being periodically output from an output end facet of the optical waveguide.

Claim 33

An apparatus according to claim 15, the optical wavelength converting device additionally including: a plurality of second inverted-polarization layers arranged in parallel to the inverted-polarization layers at second regular intervals to cross the optical waveguide, polarization of the second inverted-polarization layers being directed toward the -C-crystal axis direction, and the second inverted-polarization layers being formed by exchanging positive ions included in the ferroelectric substrate for H + ions; and a first electrode arranged on the ferroelectric substrate and the second inverted-polarization layers positioned in the +C-crystal axis direction to the optical waveguide; a second electrode arranged on the ferroelectfic substrate and the second inverted-polarization layers positioned in the -C-crystal axis direction to the optical waveguide; and an electric source for applying an electric potential difference between the first and second electrodes to induce electric field through the optical waveguide between the first and second electrodes, a first refractive index of the second inverted-polarization layers in the optical waveguide and a second refractive index of the ferroelectric substrate in the optical waveguide being changed according to intensity of the electric field on condition that increase or decrease of the first refractive index is opposite to that of the second refractive index to produce a diffraction grating formed of alternate changes of the first and second refractive indexes in the optical waveguide, the coherent light of a particular wavelength being selectively reflected by the diffraction grating, and the coherent light reflected being returned to the semiconductor laser to fix the wavelength of the coherent light radiated from the semiconductor laser to the particular wavelength.