JPS604961B2 - optical waveguide device - Google Patents
optical waveguide deviceInfo
- Publication number
- JPS604961B2 JPS604961B2 JP51005609A JP560976A JPS604961B2 JP S604961 B2 JPS604961 B2 JP S604961B2 JP 51005609 A JP51005609 A JP 51005609A JP 560976 A JP560976 A JP 560976A JP S604961 B2 JPS604961 B2 JP S604961B2
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- optical waveguide
- optical
- crystal
- substrate
- 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.)
- Expired
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- Optical Integrated Circuits (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
Description
【発明の詳細な説明】
本発明は光集積回路等における光導波装置に関し、Pb
Mo04のようなAB04形正万晶構造をもつ酸化物単
結晶を基板として、その上にZnTe、ZnSe、ある
いはその混晶などのローの族立方晶系化合物半導体薄膜
を異種接合して光導波のための光導波装置を形成し、種
々の光集積回路の機能素子への応用に供することを目的
とする。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical waveguide device in an optical integrated circuit, etc.
An oxide single crystal with an AB04-type regular crystal structure such as Mo04 is used as a substrate, and a low group cubic compound semiconductor thin film such as ZnTe, ZnSe, or a mixed crystal thereof is bonded to the substrate to form an optical waveguide. The purpose of this invention is to form an optical waveguide device for use in various optical integrated circuit functional elements.
将来の大容量光学通信システムは種々の能動的及び受動
的集積光学回路装置を有し、情報をのせた光波を導き処
理を行なう機能をもつものである。Future high-capacity optical communication systems will include a variety of active and passive integrated optical circuit devices capable of guiding and processing information-carrying light waves.
最近そのために種々の薄膜光導波路、光集積回路の研究
がなされている。Recently, various thin film optical waveguides and optical integrated circuits have been studied for this purpose.
現在までのこの分野の研究により前記光学システムが成
功するかどうかは適当な光伝送特性を持ち、導波処理を
有する装置の製造に最適な薄膜材料の開発に依存する。
現在単結晶薄膜材料としては一般的に光導波損失が小さ
く、希望する性質と形状の製造が簡単で安価であり、能
動素子の作製についてもよく適応できる。例えば、Lj
Nb03、GaAs−GaAIAs、各種ガーネット薄
膜単結晶などが研究され、薄膜光スイッチ、変調器、レ
ーザーなどの素子が報告されている。しかしこれらの最
近の開発研究にもかかわらず光の損失、変調等の点で光
薄膜装置に適する単結晶材料はまれである。したがって
、今日前記光学システムで多くの種類の能動的、受動的
素子の作製に適する新らしい単結晶材料に対する要求が
高まっている。ところでロー町族化合物半導体は半導体
の中でも電気光学効果が大きく、ZnSe、ZnTeの
単結晶板を使用した光変調器の報告がある。Based on research in this field to date, the success of such optical systems depends on the development of thin film materials with suitable light transmission properties and suitable for the fabrication of devices with waveguide processing.
Currently, single-crystal thin film materials generally have low optical waveguide loss, are easy and inexpensive to manufacture with desired properties and shapes, and are well suited for the production of active devices. For example, Lj
Nb03, GaAs-GaAIAs, various garnet thin film single crystals, etc. have been studied, and devices such as thin film optical switches, modulators, and lasers have been reported. However, despite these recent developments and studies, single crystal materials suitable for optical thin film devices are rare in terms of optical loss, modulation, etc. Therefore, there is an increasing demand today for new single crystal materials suitable for the fabrication of many types of active and passive components in said optical systems. By the way, Rhoch group compound semiconductors have a large electro-optic effect among semiconductors, and there are reports of optical modulators using single crystal plates of ZnSe and ZnTe.
しかし薄膜単結晶の例はみあたらず、単にZnTe−G
a船のごとく半導体へテロ接合として単結晶薄膜が作成
された例があるのみで、このZnTe−GaASはGa
ASの屈折率の方が大きいため光素子用に適したZnT
e結晶に光をとじ込めることができず、光導波装置とし
て用いることはできない。そこで本発明は上司ZnSe
、ZnTe等のロー町族化合物半導体結晶を用いるとと
もに、この単結晶薄膜をそれより低い屈折率を有する一
般的にAB04型(ただし、AはPb、Ca、Sr、B
aより選ばれた1つ、BはMo、Wより選ばれた1つ)
正方晶系横造をもつ単結晶基板上に形成し、ここで形成
された単結晶薄膜に光導波路を形成することにより、す
ぐれた光伝送特性を得るものである。すなわち、PbM
o04やCaW04などの正方晶系構造をもつAB04
型の酸化物は今まで単結晶や粉末の形で扱かわれてきて
おり、音響光学素子として、また蟹光体、レーザの母体
材料として研究されてきた。このAB04型の結晶は光
の屈折率がZnTe、ZnSe等のローの族化合物半導
体よりも小さく、このA804型結晶基板上に上記0一
町族化合物半導体単結晶薄膜を成長させると、この薄膜
に光が有効にとじ込められ、電気光学効果が大で損失も
小さいすぐれた光導波路を得ることができる。さて、A
B04型結晶とZnSe、ZnTe、ZnSなどのロー
町族半導体結晶の結晶学的性質を次表に示す。この表よ
り、0−の族半導体結晶とA804型縞晶との接合をみ
ると格子定数のズレの程度は14%程度以下となってい
てェピタキシアル成長が可能な範囲であり、結晶構造的
にはAB04型結晶の(001)面と半導体結晶の{1
00}面とで最も良好なェピタキシアル成長を得ること
ができる。However, there are no examples of thin film single crystals, and it is simply ZnTe-G.
There is only one example of a single crystal thin film being created as a semiconductor heterojunction, such as in the A ship, and this ZnTe-GaAS is
ZnT is suitable for optical devices because its refractive index is higher than that of AS.
It is not possible to trap light in the e-crystal, and it cannot be used as an optical waveguide device. Therefore, the present invention is based on the boss ZnSe.
, ZnTe, etc. are used, and this single crystal thin film is generally of the AB04 type (where A is Pb, Ca, Sr, B
One selected from a, B is Mo, one selected from W)
Excellent optical transmission characteristics can be obtained by forming an optical waveguide on a single crystal thin film formed on a single crystal substrate with a tetragonal horizontal structure. That is, PbM
AB04 with a tetragonal structure such as o04 and CaW04
Until now, oxides of this type have been treated in the form of single crystals or powders, and have been studied as acousto-optic devices and as base materials for crab optics and lasers. This AB04 type crystal has a light refractive index smaller than that of low group compound semiconductors such as ZnTe and ZnSe, and when the above 01 group compound semiconductor single crystal thin film is grown on this A804 type crystal substrate, this thin film It is possible to obtain an excellent optical waveguide in which light is effectively confined, the electro-optic effect is large, and the loss is small. Now, A
The following table shows the crystallographic properties of B04 type crystals and low-choice group semiconductor crystals such as ZnSe, ZnTe, and ZnS. From this table, looking at the junction between the 0- group semiconductor crystal and the A804 type striped crystal, the degree of lattice constant deviation is about 14% or less, which is within the range where epitaxial growth is possible, and in terms of the crystal structure. (001) plane of AB04 type crystal and {1 of semiconductor crystal
00} plane, the best epitaxial growth can be obtained.
また熱膨脹係数の差はローW族半導体−A804結晶の
それは現在ェピタキシアルで成功しているサファイア上
のSiのそれに比して小さく、冷却による熱歪としては
小さくなる。上記表の屈折率比較からローW族半導体結
晶はA804結晶よりも屈折率が高く、半導体結晶薄膜
の膜厚がその平面と平行な誘導モードで薄膜中を伝播す
る光の波長にほぼ近いオーダーの大きさの厚みを持つ時
、高品位な光導波のための光導波装置を構成することが
できる。光導波路用薄膜は本来、その中を伝播する光の
波長のオーダーの厚みを有すれば良く、薄膜の厚さは光
波長の0.1〜ION音の範囲のものを得ることができ
るが、波長の1〜1び音の範囲が良好である。Furthermore, the difference in coefficient of thermal expansion of the low W group semiconductor-A804 crystal is smaller than that of Si on sapphire, which is currently successful in epitaxial formation, and the thermal strain due to cooling is small. From the refractive index comparison in the table above, the low W group semiconductor crystal has a higher refractive index than the A804 crystal, and the thickness of the semiconductor crystal thin film is on the order of approximately close to the wavelength of light propagating in the thin film in the guided mode parallel to its plane. When the thickness is large enough, an optical waveguide device for high-quality optical waveguide can be constructed. Originally, a thin film for an optical waveguide only needs to have a thickness on the order of the wavelength of the light propagating therein, and the thickness of the thin film can range from 0.1 of the optical wavelength to ION sound. The wavelength range of 1 to 1 digit is good.
光導波の実験は良く知られているプリズム光結合器によ
り第1図の如くし−ザー光を薄膜中へ導入することによ
り行われる。第1図において1は基板、2は光導波用ェ
ピタキシアル薄膜、3,3′はプリズム結合器、4はし
ーザー光である。この方法により光損失の値を求め薄膜
の良否を判定することができる。さて、上記AB04型
結晶にェピタキシアル成長によりローの族半導体結晶薄
膜を得る本発明の実施例を説明する。Optical waveguide experiments are carried out by introducing laser light into a thin film using a well-known prism optical coupler as shown in FIG. In FIG. 1, 1 is a substrate, 2 is an epitaxial thin film for optical waveguide, 3 and 3' are prism couplers, and 4 is a laser beam. By this method, it is possible to determine the value of optical loss and determine the quality of the thin film. Now, an embodiment of the present invention will be described in which a rho group semiconductor crystal thin film is obtained by epitaxial growth on the AB04 type crystal.
{1’PbMo04、欧W04上へのZnSeの黍着P
bMo04の(001)面を基板としてZnSe単結晶
を蒸発源として蒸着を行なった。{1'PbMo04, ZnSe deposition on European W04P
Vapor deposition was performed using the (001) plane of bMo04 as a substrate and a ZnSe single crystal as an evaporation source.
基板温度は200oo〜600qoまで変化させ、蒸着
温度は800℃〜1000ooで行なった。基板温度は
400oo〜500午○でかなり良好なェピタキシアル
膜を得ることができ、光導波のテストでも損失は小さく
、磯W04でもほぼ同じ結果が得られる。The substrate temperature was varied from 200oo to 600qo, and the deposition temperature was from 800°C to 1000o. A fairly good epitaxial film can be obtained at a substrate temperature of 400 to 500 pm, and the loss is small in the optical waveguide test, and almost the same results can be obtained with Iso W04.
■ PbMo04上へのZnTeの成長
PbMo04の(001)面を基板として第2図に示す
成長装置で気相成長させた。(2) Growth of ZnTe on PbMo04 Using the (001) plane of PbMo04 as a substrate, vapor phase growth was performed using the growth apparatus shown in FIG.
加熱炉5中の石英管6中で、Zn、Teの原料7,8側
の温度は49000一定とし、Zn、Teガスの供給量
は日2ガス流量を変化させて制御する。PbMo04基
板9の温度720℃、主H2流量200cc′min、
ZnとTeのキャリアガス流量50cc′minで行な
った時、数千Aから100仏程の厚さの成長層を得た。
成長層はX線及び電子線回折によって単結晶薄膜である
ことが確認されるとともに、PbMo04結晶(001
)面にZnTe(100)が成長していた。光導波テス
トについても良好であった。〔3l PbMo04上へ
のZnSe,NTex(0<×<1)の蒸着PbMo0
4の(001)面を基板としてZnSeo.5Teo.
5を蒸発材料として蒸着を行なった。In the quartz tube 6 in the heating furnace 5, the temperature on the side of the Zn and Te raw materials 7 and 8 is kept constant at 49,000, and the supply amount of the Zn and Te gases is controlled by changing the gas flow rate twice a day. PbMo04 substrate 9 temperature 720°C, main H2 flow rate 200cc'min,
When this was carried out at a carrier gas flow rate of 50 cc'min for Zn and Te, a grown layer with a thickness of several thousand amps to about 100 amps was obtained.
The grown layer was confirmed to be a single crystal thin film by X-ray and electron diffraction, and it was confirmed that it was a PbMo04 crystal (001
) ZnTe (100) was grown on the surface. The optical waveguide test also performed well. [3l Vapor deposition of ZnSe, NTex (0<x<1) on PbMo04
Using the (001) plane of ZnSeo.4 as a substrate, ZnSeo. 5Teo.
5 was used as the evaporation material.
条件は実施例{1ーとほぼ同等であり、得られた膜は部
分的に単結晶化しており光導波テストでは{1}より損
失は少し大きい値が得られた。xの範囲値はZnSe,
‐xTex混晶単結晶作製例と同等の値が得られる。Z
nSe、ZnTeは他にPbW04、SrW04、Sr
Mo04、母W04上へのェピタキシアルがX線及び電
子線回折により確認された。本発明は上記実施例のェピ
タキシアル方法にのみよらず、ェピタキシアル方法とし
ては液相、気相、分子線ェピタキシアル、真空蒸着法な
どが適用できる。The conditions were almost the same as in Example {1--, and the obtained film was partially single crystallized, and the optical waveguide test showed a slightly larger loss than in {1}. The range value of x is ZnSe,
- The same value as the xTex mixed crystal single crystal production example can be obtained. Z
In addition to nSe and ZnTe, PbW04, SrW04, and Sr
Epitaxial formation on Mo04 and mother W04 was confirmed by X-ray and electron diffraction. The present invention is not limited to the epitaxial method of the above-mentioned embodiments, but can also be applied to liquid phase, gas phase, molecular beam epitaxial, vacuum evaporation methods, and the like.
本発明の光導波装置はD−W族化合物半導体の持つ特性
、即ち、一般に良く知られている電気光学効果を使用し
た第3,4図に示す光変調器、光スイッチあるいは光伝
導性を使用する第5,6図のフオトディテクターなどを
構成することができる。The optical waveguide device of the present invention uses the characteristics of D-W group compound semiconductors, that is, the optical modulator, optical switch, or photoconductivity shown in FIGS. 3 and 4 that uses the generally well-known electro-optic effect. A photodetector such as that shown in FIGS. 5 and 6 can be constructed.
第3,4図において、9はAB04型単結晶基板、10
Gま基板9上に成長されたローの族半導体単結晶薄膜、
11,12はこの薄膜に不純物を拡散して形成された光
導波路13,14,15は電極であって、この電極14
に電源16より電圧を印加して第3,4図に示す光変調
器が構成されており、薄膜11と12は方向性光結合器
を形成している。In Figures 3 and 4, 9 is an AB04 type single crystal substrate, 10
A low group semiconductor single crystal thin film grown on a substrate 9;
Optical waveguides 13, 14 and 15 formed by diffusing impurities into this thin film are electrodes 11 and 12, and this electrode 14
A voltage is applied from a power supply 16 to the optical modulator shown in FIGS. 3 and 4, and the thin films 11 and 12 form a directional optical coupler.
すなわち半導波路11に入射された光17は電極への印
加電圧より変調され導波路により出力させる。第6,6
図において、9,10,11は第3図と同一のものを示
し、薄膜11と電極20,21とでショットキバリア形
フオトダィオード部を構成している。That is, the light 17 incident on the semi-waveguide 11 is modulated by the voltage applied to the electrodes and output from the waveguide. 6th, 6th
In the figure, numerals 9, 10, and 11 are the same as in FIG. 3, and the thin film 11 and electrodes 20 and 21 constitute a Schottky barrier photodiode section.
22,23は引き出しリード線である。22 and 23 are lead wires.
この装置は薄膜11を通ってきた光を上記フオトダィオ
ード部で検出するものである。以上のように本発明はロ
ーの族化合物半導体の薄膜をAB04形正方晶結晶絶縁
体基板上に形成し、光導波のための光導波装置の作成を
可能とするもので、基板の選択や固溶体化により欠陥の
少い結晶性の良好な薄膜単結晶ができ、それゆえ良好な
薄膜光導波装置を可能とするものである。This device detects light passing through the thin film 11 using the photodiode section. As described above, the present invention enables the creation of an optical waveguide device for optical waveguide by forming a thin film of a rho group compound semiconductor on an AB04 type tetragonal crystal insulator substrate. By this process, a thin film single crystal with few defects and good crystallinity can be produced, thereby making possible a good thin film optical waveguide device.
すなわち、D−W族結晶の高い電気光学効果により、光
変調器、光スイッチが作製出来、ショットキーバリャ型
の光検出器、ヘテロ接合型のフオトダィオードが同一基
板上に可能となり、光通信のための信号処理部品として
有益な装置を供するものである。In other words, the high electro-optic effect of D-W group crystals makes it possible to fabricate optical modulators and optical switches, as well as Schottky barrier photodetectors and heterojunction photodiodes on the same substrate, making it possible for optical communication. The present invention provides a device useful as a signal processing component for a computer.
第1図は光導波実験用プリズム光結合器の構造断面図、
第2図は本発明の一実施例で使用する気相成長装置の概
略構成図、第3図は本発明を応用した光変調器の平面図
、第4図は第3図のm−m′線断面図、第5図は同じく
本発明を応用したフオトディテクターの要部断面図、第
6図は第5図のV−V′線断面図である。
9・・・・・・AB04型単結晶基板、1 0,1 1
・…・・ロー町族化合物半導体単結晶薄膜。
第1図
第2図
第3図
第4図
第5図
第6図Figure 1 is a cross-sectional view of the structure of a prism optical coupler for optical waveguide experiments.
FIG. 2 is a schematic configuration diagram of a vapor phase growth apparatus used in an embodiment of the present invention, FIG. 3 is a plan view of an optical modulator to which the present invention is applied, and FIG. 4 is a line m-m' in FIG. 5 is a sectional view of a main part of a photodetector to which the present invention is applied, and FIG. 6 is a sectional view taken along the line V-V' in FIG. 9...AB04 type single crystal substrate, 1 0, 1 1
...Rhocho group compound semiconductor single crystal thin film. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6
Claims (1)
aの群より選択された1つ、BはMo、Wの群より選択
された1つ)の正方晶酸化物基板上に、上記基板より光
学的屈折率の大きなII−VI族立方晶系化合物半導体単結
晶薄膜を形成し、この薄膜の所定部に光導波路を形成し
たことを特徴とする光導波装置。 2 上記ABO_4型結晶の(001)面上に、上記化
合物半導体の{100}面をエピタキシヤル成長させた
ことを特徴とする特許請求の範囲第1項に記載の光導波
装置。 3 上記化合物半導体がZnSe、ZnTe、ZnSe
_1_−_xTe_x(0<x<1)、ZnSよりなる
ことを特徴とする特許請求の範囲第1項に記載の光導波
装置。[Claims] 1 ABO_4 type (A: Pb, Ca, Sr, B
A group II-VI cubic compound having a larger optical refractive index than the substrate is placed on a tetragonal oxide substrate (one selected from the group a, B is one selected from the group of Mo and W). An optical waveguide device characterized in that a semiconductor single crystal thin film is formed and an optical waveguide is formed in a predetermined portion of this thin film. 2. The optical waveguide device according to claim 1, wherein the {100} plane of the compound semiconductor is epitaxially grown on the (001) plane of the ABO_4 type crystal. 3 The above compound semiconductor is ZnSe, ZnTe, ZnSe
_1_-_xTe_x (0<x<1), the optical waveguide device according to claim 1, characterized in that it is made of ZnS.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51005609A JPS604961B2 (en) | 1976-01-20 | 1976-01-20 | optical waveguide device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51005609A JPS604961B2 (en) | 1976-01-20 | 1976-01-20 | optical waveguide device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5288353A JPS5288353A (en) | 1977-07-23 |
| JPS604961B2 true JPS604961B2 (en) | 1985-02-07 |
Family
ID=11615934
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP51005609A Expired JPS604961B2 (en) | 1976-01-20 | 1976-01-20 | optical waveguide device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS604961B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6035270U (en) * | 1983-08-19 | 1985-03-11 | 三菱自動車工業株式会社 | Potentiometer type sensor disconnection detection circuit |
| JPH0271275U (en) * | 1988-11-18 | 1990-05-30 |
-
1976
- 1976-01-20 JP JP51005609A patent/JPS604961B2/en not_active Expired
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6035270U (en) * | 1983-08-19 | 1985-03-11 | 三菱自動車工業株式会社 | Potentiometer type sensor disconnection detection circuit |
| JPH0271275U (en) * | 1988-11-18 | 1990-05-30 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5288353A (en) | 1977-07-23 |
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