JPS6057825A - Light wavelength converting element - Google Patents

Light wavelength converting element

Info

Publication number
JPS6057825A
JPS6057825A JP16697383A JP16697383A JPS6057825A JP S6057825 A JPS6057825 A JP S6057825A JP 16697383 A JP16697383 A JP 16697383A JP 16697383 A JP16697383 A JP 16697383A JP S6057825 A JPS6057825 A JP S6057825A
Authority
JP
Japan
Prior art keywords
light
optical
optical waveguide
light guide
wavelength
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP16697383A
Other languages
Japanese (ja)
Other versions
JPH0426085B2 (en
Inventor
Kazuhisa Yamamoto
和久 山本
Tetsuo Taniuchi
哲夫 谷内
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP16697383A priority Critical patent/JPS6057825A/en
Publication of JPS6057825A publication Critical patent/JPS6057825A/en
Publication of JPH0426085B2 publication Critical patent/JPH0426085B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/35Non-linear optics
    • G02F1/37Non-linear optics for second-harmonic generation
    • G02F1/377Non-linear optics for second-harmonic generation in an optical waveguide structure

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Integrated Circuits (AREA)
  • Liquid Crystal (AREA)

Abstract

PURPOSE:To improve the efficiency of SHG (2nd higher harmonic generation) conversion by forming a light guide which is longer than a substrate in an X and an Y axial direction on the Z surface of nonlinear optical crystal having an X, an Y, and a Z axis. CONSTITUTION:The light guide which is 6mum wide and 4mum deep is formed by diffusing thermally Ti in the Z surface of the LiNbO3Z plate 3' which is, for example, 2cm in the X axial direction and 1cm long in the Y axial direction. Light with wavelength lambda is made incident on this light guide 4a from its incidence end part 5 and reflected by a reflecting end part 6 where a metallic film is vapor-deposited to propagate to the next light guide 4b. The light guides (a) and (b) are at a 3 deg. angle to each other. Light entering the light guide 4c similarly is projected from a projection end part 7. The overall length of the light guides is about 6cm. Then, the incident light with the wavelength lambda and light of a converted wave with wavelength lambda/2 are put in phase with each other to maximize the output power of the converted wave. In practice, semiconductor laser light which has 1.3mum wavelength and 40mW output power is converged by a lens, made incident on the incidence end part 5, and put in phase by temperature to obtain a bit over 20% conversion efficiency.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、レーザ光を使用する情報処理分野あるいは光
応用計測制御分野に利用する光波長変換素子に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to an optical wavelength conversion element used in the information processing field or optical applied measurement control field using laser light.

従来例の構成とその問題点 従来、0.7μm以下の短波長領域においては半導体レ
ーザによる発振が困難であるため、気体レーザなどの大
型レーザが使われており、大型化がさけられなかった。
Conventional Structures and Problems Conventionally, it has been difficult for semiconductor lasers to oscillate in the short wavelength region of 0.7 μm or less, so large lasers such as gas lasers have been used, and larger lasers have been unavoidable.

そのため5HG(第2高調波発生)現象を利用し半導体
レーザ光を半分の波長に変換する素子が作製されていた
。第1図は従来のL iN b03光導波路を使用した
光波長変換素子によシ半導体レーザ光を変換する構成を
示した斜視図である。半導体レーザ1から出た波長λの
光はレンズ2によシ集光されてL iN b Oa Y
板3に形成された光導波路4に入る。この波長λの半導
体レーザよシの入射光と変換された波長λ/2の光の位
相整合条件をL z N b O3ル爬銘4帽を変える
などの方法により満たしてやることにより数パーセント
の変換効率で波長λ/2の変換光を得ていた。実際にL
 z N b O3Y板3に幅6 It m 、深さ1
.5μm長さ2CmのTf拡散光4波路4全作製し、波
長1.3μm、出力40’ m Wの半導体レーザの光
全党導波路4に入射することにより、2%の変換効率で
波長0.66μmの変換光が得られている。しかし、変
換効率は光4波路4のアスペクト比(幅と深さの比)が
1に近い程良く、LiNb○3Y板3ではX軸方向の拡
散係数が太きいために、光4波路4が大きく横に広がっ
てしまめ変換子が極端に悪くなる。また変換効率は光導
波路4の長さの二乗に比例するのであるが、変換効率を
上げようとした場合、X軸方向のLiNb○3Y板3の
長さを長くとらなければならず、光波長変換素子の大き
さが大きくなってし甘う。
For this reason, elements have been manufactured that utilize the 5HG (second harmonic generation) phenomenon to convert semiconductor laser light into half the wavelength. FIG. 1 is a perspective view showing a configuration for converting semiconductor laser light by an optical wavelength conversion element using a conventional LiN b03 optical waveguide. Light with wavelength λ emitted from semiconductor laser 1 is focused by lens 2 and becomes L iN b Oa Y
It enters an optical waveguide 4 formed in the plate 3. By satisfying the phase matching condition between the incident light of the semiconductor laser of wavelength λ and the converted light of wavelength λ/2 by a method such as changing the LzNbO3 head, a conversion of several percent can be achieved. Converted light of wavelength λ/2 was obtained with efficiency. Actually L
z N b Width 6 It m, depth 1 on O3Y plate 3
.. By fabricating four Tf diffused light waveguides 4 with a length of 5 μm and a length of 2 Cm, and inputting the light into the optical waveguide 4 of a semiconductor laser with a wavelength of 1.3 μm and an output of 40' mW, a conversion efficiency of 2% and a wavelength of 0. Converted light of 66 μm was obtained. However, the conversion efficiency is better as the aspect ratio (width to depth ratio) of the four optical wave paths 4 is closer to 1, and since the LiNb○3Y plate 3 has a large diffusion coefficient in the X-axis direction, the four optical wave paths 4 are It spreads wide and the shimeme converter becomes extremely bad. Furthermore, the conversion efficiency is proportional to the square of the length of the optical waveguide 4, but in order to increase the conversion efficiency, it is necessary to increase the length of the LiNb○3Y plate 3 in the X-axis direction, which increases the optical wavelength. The size of the conversion element is too large.

発明の目的 本発明の目的は、x、y、z各軸を有する非線形光学結
晶のZ板を用いることに」:す、Z面VC形成された光
導波路のアスペクト比を1Vこ近付け、さらに上記光導
波路を折り返しまた曲りl′l′4造にして光導波路の
長さをかせぐことにより、従来では困鄭、であった変換
効率を太きく1コげるコン・くクトな光波長変換素子を
提供することにある。
OBJECTS OF THE INVENTION An object of the present invention is to use a Z plate of nonlinear optical crystal having x, y, and z axes, to bring the aspect ratio of the optical waveguide formed in the Z-plane VC closer to 1V, and to further achieve the above-mentioned By folding or bending the optical waveguide to increase the length of the optical waveguide, a compact optical wavelength conversion element that greatly increases the conversion efficiency, which was difficult to achieve in the past. Our goal is to provide the following.

発明の構成 本発明の光波長変換素子は、X 、 Y 、 Z@軸を
有する非線形光学結晶の2面に、前記x、y軸方向の長
さよりも長い光導波路を設けた構成である。
Configuration of the Invention The optical wavelength conversion element of the present invention has a configuration in which optical waveguides longer than the lengths in the x and y axis directions are provided on two surfaces of a nonlinear optical crystal having X, Y, and Z@ axes.

また本発明の光波長変換素子は上記非線光学結晶としテ
L I N b O12板、LiTa03Z板を用いj
c n’lJRである。また本発明の光波長変換素子は
上記光導波路として全反射または方向性結合による折り
返し光導波路、または曲シ光導波路を用いた’4tj 
I戊である。
Furthermore, the optical wavelength conversion element of the present invention uses the above-mentioned non-linear optical crystals, such as TeLINbO12 plate and LiTa03Z plate.
c n'lJR. Further, the optical wavelength conversion element of the present invention uses a folded optical waveguide by total reflection or directional coupling, or a curved optical waveguide as the optical waveguide.
It is I.

実施例の説明 第2図は、本発明による光波」〈変換1子の第1の実施
例の構成を示した斜視図である。第21図において、X
軸方向に2 Cm * Y’1u11方向に1 cmの
長さを1.5″ったL I N b Os Z板3′の
Z而にTiを熱波11夕することによシ幅6μm、深さ
4μmの光導波路4a′ff:形成した。この光導波路
4aに入射端部6よシ波長λの光が入射され、この光は
金属膜が蒸着さ九た反射端部6で反射され、次の光導波
路4bに移る。光導波路aと先導波路すは3°の角度を
もたせである。同様の過程を経て光導波路4Cに入った
光は出射端部7よシ出射する。全光導波路の長さはほぼ
ecmとなる。
DESCRIPTION OF THE EMBODIMENTS FIG. 2 is a perspective view showing the structure of a first embodiment of the light wave converter according to the present invention. In Figure 21,
By applying heat waves to Ti on the Z of the L I N b Os Z plate 3' with a length of 1.5'' and 2 cm in the axial direction and 1 cm in the Y'1u11 direction, a width of 6 μm was formed. An optical waveguide 4a'ff with a depth of 4 μm was formed. Light with a wavelength λ is incident on this optical waveguide 4a from the input end 6, and this light is reflected at the reflective end 6 on which the metal film is vapor-deposited. Moving on to the next optical waveguide 4b.The optical waveguide a and the leading waveguide A are at an angle of 3 degrees.The light that enters the optical waveguide 4C through the same process is output from the output end 7.All optical waveguides The length of is approximately ecm.

ここで波長λの入射光の光と波長λ/2変換波の光との
位相を温度などにより整合させることにより、変換波の
出力パワーを最大にすることができる。実際には波長1
.3μm、出力パワー4c)mWの半導体レーザ光をレ
ンズで集光して入射端部5より入射させ、温度により位
届ヲ整合させることで20%強の変換効率が得られた。
Here, the output power of the converted wave can be maximized by matching the phases of the incident light having the wavelength λ and the wavelength λ/2 converted wave using temperature or the like. Actually wavelength 1
.. A conversion efficiency of over 20% was obtained by condensing a semiconductor laser beam of 3 μm and output power of 4 c) mW with a lens, making it incident through the input end 5, and adjusting the position depending on the temperature.

第3図は、本発明による光波長変換素子の第2の実施例
を示した斜視図である。L I N b O3Z板3′
に設けられた光導波路4aと4b、4bと4c間の結合
は完全結合長を持った方向性結合によって行っている以
外は実施例1と同様である。
FIG. 3 is a perspective view showing a second embodiment of the optical wavelength conversion element according to the present invention. L I N b O3Z board 3'
The optical waveguides 4a and 4b, 4b and 4c provided in the optical waveguides 4a and 4b are coupled to each other in the same way as in the first embodiment except that the coupling is performed by directional coupling with a perfect coupling length.

s A Ill ++ 太gト日日W F Z、−W−
?rl!↓L 亦’、! $二i’−77)4’ff 
Qの実施例を示した斜視図である。この実施例では折り
返し導波路を用いる代りに、曲り光導波路として渦巻き
光導波路4を用いて波長変換素子を構成した。LiNb
○3Y板では曲りを付けることにまり伝搬定数が変化し
位相整合条件が各場所によシ異なるが、L x N b
 Os Z板を用いているため伝搬定数は変化しないの
で位相整合条件は場所によシ異ならない。光導波路4は
全長5cmである。この光導波路4′に波長0.8μm
、出力パワー30mWの半導体レーザ光全入射させ、温
度により位相を整合させたところ15%の変換効率で波
長0.4μmの変換光が得られた。
s A Ill ++ Thick day day W F Z, -W-
? rl! ↓L 亦'、! $2i'-77)4'ff
It is a perspective view showing an example of Q. In this embodiment, instead of using a folded waveguide, a spiral optical waveguide 4 was used as a curved optical waveguide to construct a wavelength conversion element. LiNb
○In a 3Y plate, the propagation constant changes due to bending, and the phase matching conditions differ depending on the location, but L x N b
Since the Os Z plate is used, the propagation constant does not change, so the phase matching conditions do not differ depending on the location. The optical waveguide 4 has a total length of 5 cm. This optical waveguide 4' has a wavelength of 0.8 μm.
When all of the semiconductor laser light with an output power of 30 mW was made incident and the phase was matched by temperature, converted light with a wavelength of 0.4 μm was obtained with a conversion efficiency of 15%.

以上実施例では結晶としてL z N b O12板を
用いたが他にL f T a Osなどx、y、z軸を
持つ非線形光学結晶であればよい。また、実施例でHx
X軸方向前記非線形光学結晶の長さの数倍の長さを持つ
光導波路を用いたが、折り返す回数を増すなどによりさ
らに光導波路長全長くして変換効率をさらにあけること
も可能である。=!、た曲り光4波路として渦巻き光導
波路を用いて説明を行ったが、U字型、S字型などこれ
に限ることはない。また本実施例ではSHGについて説
明を行ったが、光バラメートリック増幅、和周波、差周
波などにも用いることができる。
In the above embodiments, an L z N b O12 plate was used as the crystal, but any other nonlinear optical crystal having x, y, and z axes, such as L f Ta Os, may be used. In addition, in the example, Hx
Although an optical waveguide having a length several times the length of the nonlinear optical crystal in the X-axis direction was used, it is also possible to further increase the conversion efficiency by increasing the total length of the optical waveguide by increasing the number of turns. =! Although the description has been given using a spiral optical waveguide as a four-wave path for curved light, the waveguide is not limited to a U-shape, an S-shape, etc. Further, in this embodiment, the SHG has been explained, but it can also be used for optical parametric amplification, sum frequency, difference frequency, etc.

発明の詳細 な説明したように、本発明の光波Jぐ変換素子において
は、X、Y、Z@軸を有する非線形光学結晶の2面に前
記X、Y軸方向の基板の長さ」;シ長い光導波路全作製
することに」:す、従来のX。
As described in detail of the invention, in the light wave converting element of the present invention, the length of the substrate in the X, Y axis directions is formed on two surfaces of the nonlinear optical crystal having In order to fully fabricate a long optical waveguide: the conventional X.

Y面に作製された光導波路に比べSHG変換効率を士数
倍程度高めることができるすぐれた効果を発揮すること
ができる。
It is possible to exhibit an excellent effect of increasing the SHG conversion efficiency by several times compared to an optical waveguide fabricated in the Y plane.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来のL I N b 03光導波路を使用し
た光波長変換素子により半導体レーザ光を変換する装置
の概略斜視図、第2図は本発明による光波長変換素子の
第1の実施例の構成全示した概略斜視図、第3図は本発
明による光波長変換素子による第2の実施例を示した概
略斜視図、第4図は本発明による光波長変換素子の第3
の実施例を示した概略斜視図である。 1・・・・・・半導体レーザ、2・・・・・レンズ、3
・・・・・・L I N b Os Y板、4a 、4
b 、4c 、4’ −=−・光導波路、3′・・パ・
・・L I N b O12板、6・・・・・入射端部
、6・・・・・・反射端部、7・・・・・・出射端部。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第 2 図 第3図 第4図 4′
FIG. 1 is a schematic perspective view of a device for converting semiconductor laser light by an optical wavelength conversion element using a conventional L I N b 03 optical waveguide, and FIG. 2 is a first embodiment of the optical wavelength conversion element according to the present invention. FIG. 3 is a schematic perspective view showing a second embodiment of the optical wavelength conversion element according to the present invention, and FIG. 4 is a schematic perspective view showing the entire configuration of the optical wavelength conversion element according to the present invention.
FIG. 2 is a schematic perspective view showing an embodiment of the invention. 1... Semiconductor laser, 2... Lens, 3
・・・・・・L I N b Os Y board, 4a, 4
b, 4c, 4' -=-・Optical waveguide, 3'...Pa・
...L I N b O12 plate, 6...Incidence end, 6...Reflection end, 7...Output end. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 Figure 3 Figure 4 Figure 4'

Claims (4)

【特許請求の範囲】[Claims] (1)X、Y、Z各軸を有する非線形光学結晶の2面に
前記X、Y軸方向の長さよシも長い光導波路を設けたこ
とを特徴とする光波長変換素子。
(1) An optical wavelength conversion element characterized in that an optical waveguide which is longer than the length in the X and Y axes directions is provided on two surfaces of a nonlinear optical crystal having each of the X, Y, and Z axes.
(2)X、Y、Z各軸を有する非線形生学結晶としてL
iNb0 Z板又はL I T a Os Z板を用い
たことを特徴とする特許請求の範囲第1項記載の光波長
変換素子。
(2) L as a nonlinear biocrystal with X, Y, and Z axes
The optical wavelength conversion element according to claim 1, characterized in that an iNb0 Z plate or a L I T a Os Z plate is used.
(3)X、Y1111方向の長さよシも長い光導波路と
して折シ返し光導波路を設けたことを特徴とする特許請
求の範囲第1項記載の光波長変換素子。
(3) The optical wavelength conversion element according to claim 1, characterized in that a folded optical waveguide is provided as the optical waveguide which is longer than the length in the X and Y1111 directions.
(4)X、Y軸方向の長さよシも長い光導波路として、
方向性結合による折シ返し光導波路を設けたことを特徴
とする特許請求の範囲第1項記載の光波長変換素子。 (ei)x、y軸方向の長さよシも長い光導波路として
、曲シ光導波路を設けたことを特徴とする特許請求の範
囲第1項記載Q光波長変換素子。
(4) As an optical waveguide that is longer than the length in the X and Y axis directions,
2. The optical wavelength conversion element according to claim 1, further comprising a folded optical waveguide by directional coupling. (ei) The Q optical wavelength conversion element according to claim 1, characterized in that a curved optical waveguide is provided as the optical waveguide which is longer than the length in the x and y axis directions.
JP16697383A 1983-09-09 1983-09-09 Light wavelength converting element Granted JPS6057825A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16697383A JPS6057825A (en) 1983-09-09 1983-09-09 Light wavelength converting element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16697383A JPS6057825A (en) 1983-09-09 1983-09-09 Light wavelength converting element

Publications (2)

Publication Number Publication Date
JPS6057825A true JPS6057825A (en) 1985-04-03
JPH0426085B2 JPH0426085B2 (en) 1992-05-06

Family

ID=15841045

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16697383A Granted JPS6057825A (en) 1983-09-09 1983-09-09 Light wavelength converting element

Country Status (1)

Country Link
JP (1) JPS6057825A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009066450A1 (en) 2007-11-21 2009-05-28 Panasonic Corporation Wavelength conversion device and image display device using same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009066450A1 (en) 2007-11-21 2009-05-28 Panasonic Corporation Wavelength conversion device and image display device using same
US8294979B2 (en) 2007-11-21 2012-10-23 Panasonic Corporation Wavelength conversion device and image display apparatus using the same

Also Published As

Publication number Publication date
JPH0426085B2 (en) 1992-05-06

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