JPH0697315B2 - Loaded directional coupler - Google Patents
Loaded directional couplerInfo
- Publication number
- JPH0697315B2 JPH0697315B2 JP59069342A JP6934284A JPH0697315B2 JP H0697315 B2 JPH0697315 B2 JP H0697315B2 JP 59069342 A JP59069342 A JP 59069342A JP 6934284 A JP6934284 A JP 6934284A JP H0697315 B2 JPH0697315 B2 JP H0697315B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- loading
- optical waveguide
- loading clad
- optical
- 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 - Fee Related
Links
- 230000003287 optical effect Effects 0.000 claims description 37
- 239000000758 substrate Substances 0.000 claims description 6
- 239000004065 semiconductor Substances 0.000 claims description 4
- 239000012535 impurity Substances 0.000 claims description 3
- 238000005530 etching Methods 0.000 description 9
- 238000005253 cladding Methods 0.000 description 8
- 239000000463 material Substances 0.000 description 6
- 230000008878 coupling Effects 0.000 description 4
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 238000003776 cleavage reaction Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005693 optoelectronics Effects 0.000 description 2
- 230000007017 scission Effects 0.000 description 2
- 229910015363 Au—Sn Inorganic materials 0.000 description 1
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 description 1
- 229910013641 LiNbO 3 Inorganic materials 0.000 description 1
- 230000008033 biological extinction Effects 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 239000003989 dielectric material Substances 0.000 description 1
- 239000002019 doping agent Substances 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 238000002955 isolation Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000000206 photolithography Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/40—Arrangement of two or more semiconductor lasers, not provided for in groups H01S5/02 - H01S5/30
- H01S5/4025—Array arrangements, e.g. constituted by discrete laser diodes or laser bar
- H01S5/4031—Edge-emitting structures
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL 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
- G02F1/00—Devices 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
- G02F1/29—Devices 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 for the control of the position or the direction of light beams, i.e. deflection
- G02F1/31—Digital deflection, i.e. optical switching
- G02F1/313—Digital deflection, i.e. optical switching in an optical waveguide structure
- G02F1/3132—Digital deflection, i.e. optical switching in an optical waveguide structure of directional coupler type
- G02F1/3133—Digital deflection, i.e. optical switching in an optical waveguide structure of directional coupler type the optical waveguides being made of semiconducting materials
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Electromagnetism (AREA)
- Optical Integrated Circuits (AREA)
Description
【発明の詳細な説明】 産業上の利用分野 本発明は光通信用部品としての光スイッチ,光変調器と
して有望である方向性結合器に関するものである。Description: TECHNICAL FIELD The present invention relates to an optical switch as a component for optical communication and a directional coupler which is promising as an optical modulator.
従来例の構成とその問題点 方向性結合器は1対の光導波路を近接して並置し光の結
合を利用するとともに、電気光学効果を有する材料を用
いれば電圧印加により光の結合度を変化することができ
光の強度変調やスイッチングを行わしめることができ
る。通常このような素子はLiNbO3等の誘電体材料で多く
作られているが半導体材料を用いた場合は半導体レーザ
ー等の発光素子や受光素子およびその他の電気素子との
一体化が可能となり光集積回路の立場から非常に有望で
ある。Configuration of conventional example and its problems In a directional coupler, a pair of optical waveguides are juxtaposed side by side to utilize light coupling, and if a material having an electro-optical effect is used, the degree of light coupling is changed by voltage application. It is possible to perform intensity modulation and switching of light. Usually, such elements are often made of dielectric materials such as LiNbO 3, but when semiconductor materials are used, it becomes possible to integrate with light-emitting elements such as semiconductor lasers, light-receiving elements, and other electrical elements. Very promising from a circuit standpoint.
通常半導体を用いた場合の方向性結合器としては変調電
力等の立場からpn接合を利用できるいわゆる装荷型方向
性結合器が最も有利である。Usually, as a directional coupler using a semiconductor, a so-called loaded directional coupler that can use a pn junction from the standpoint of modulation power is most advantageous.
第1図に長波長レーザー材料であるInP/InGaAsP系を用
いた場合の方向性結合器の断面図を示す。これはSドー
プのn+InP基板1上にTeドープn+InPバファー層2,ノンド
ープのn-InGaAsP光導波層3,ZnドープのP+InPクラッド層
4を順次エピタキシャル成長し、P+InP側にAu−Zn電極
5,n+InP基板1側にAu−Sn電極6を形成したのち、P+InP
クラッド層4を導波路パターンを残してHCl系のエッチ
ャントで選択的にエッチングしてとり除き装荷クラッド
4,4′を形成し、さらにへき開により入射端面11出射端
面を形成したものである。n-InGaAsP光導波層3のう
ち、この装荷クラッド4,4′の真下の部分が三次元導波
路7,7′を形成する。FIG. 1 shows a cross-sectional view of a directional coupler using an InP / InGaAsP system, which is a long-wavelength laser material. This is a Te-doped n + InP buffer layer 2, a non-doped n - InGaAsP optical waveguide layer 3, and a Zn-doped P + InP clad layer 4 which are sequentially epitaxially grown on an S-doped n + InP substrate 1 and then grown on the P + InP side. Au-Zn electrode
5, n + InP After forming Au-Sn electrode 6 on the substrate 1 side, P + InP
The cladding layer 4 is removed by selectively etching it with an HCl-based etchant leaving the waveguide pattern.
4, 4'are formed, and then the incident end face 11 and the output end face are formed by cleavage. In the n - InGaAsP optical waveguide layer 3, the portions directly under the loaded claddings 4, 4'form the three-dimensional waveguides 7, 7 '.
ここで一方の三次元導波路7′に光を入射すると三次元
導波路7,7′間での光波の結合により、隣の導波路7に
移行する。さらに一方のAu/Zn電極5,5′と裏面のAu/Sn
電極6にpn接合に逆バイアスがかかるように電圧を印加
すると電気光学効果による導波路間の結合状態の変化に
より出射光9,9′のパワー比が変化でき光の変調および
スイッチングをおこなうことができる。Here, when light is incident on one of the three-dimensional waveguides 7 ', the light waves are coupled between the three-dimensional waveguides 7 and 7', and the light is transferred to the adjacent waveguide 7. Furthermore, one Au / Zn electrode 5, 5'and the Au / Sn on the back surface
When a voltage is applied to the electrode 6 so that a reverse bias is applied to the pn junction, the power ratio of the emitted light 9 and 9'can be changed by the change of the coupling state between the waveguides due to the electro-optical effect, and the modulation and switching of the light can be performed. it can.
ところでこの光の変調を有効に行なうためには一対の導
波路7,7′は電気的に分離されていなければならない。
しかしながら実際にはエピタキシャル成長中にn-InGaAs
P光導波層3中にP型ドーパントがオートドープされpn
接合面はn-InGaAsP光導波層3内部に形成される。従っ
て第1図に示す素子構造ではリーク電流が大きく、あま
り大きい逆バイアスは印加できない。さらに2つの導波
路7,7′は電気的に分離されておらず、一本の導波路に
独立に電圧を印加することができず、良好な光変調特性
が得られない。By the way, in order to effectively modulate this light, the pair of waveguides 7 and 7'must be electrically separated.
However, in reality, during epitaxial growth, n - InGaAs
P-type dopant is auto-doped in the P optical waveguide layer 3
The junction surface is formed inside the n − InGaAsP optical waveguide layer 3. Therefore, in the device structure shown in FIG. 1, the leak current is large and a too large reverse bias cannot be applied. Further, the two waveguides 7 and 7'are not electrically separated from each other, so that a voltage cannot be independently applied to one waveguide, and good optical modulation characteristics cannot be obtained.
このような構造の素子で電気的分離を完全におこなうた
めには装荷クラッドをエッチングする際にn-InGaAsP光
導波層3をPn接合面以下までさらにエッチングしなけれ
ばならない。しかしながら光導波層3をエッチングする
と導波路7,7′の形状が変化し、導波路間での光の結合
が弱くなり隣の導波路に光が移行するのに非常に長い距
離を要する。またエッチングのばらつき等により導波路
パラメーターを一定に保つことはむつかしい。従ってIn
Pクラッド層4,4′とInGaAsP光導波層3界面でエッチン
グをストップさせ、かつ一対の導波路を電気的に分離す
ることが望ましい方法である。In order to achieve complete electrical isolation in the device having such a structure, it is necessary to further etch the n -- InGaAsP optical waveguide layer 3 down to the Pn junction surface when etching the loading clad. However, when the optical waveguide layer 3 is etched, the shapes of the waveguides 7 and 7'change, the coupling of the light between the waveguides is weakened, and it takes a very long distance for the light to move to the adjacent waveguide. Further, it is difficult to keep the waveguide parameters constant due to variations in etching. Therefore In
It is a desirable method to stop the etching at the interface between the P clad layers 4 and 4'and the InGaAsP optical waveguide layer 3 and electrically separate the pair of waveguides.
このようにして第1図に示す構造の装荷型方向性結合器
ではpn接合面が光導波層3内部に形成されるために各導
波路に独立に電界を印加することができず、良好な光変
調特性を得ることができなかった。As described above, in the loading type directional coupler having the structure shown in FIG. 1, since the pn junction surface is formed inside the optical waveguide layer 3, it is not possible to apply an electric field to each waveguide independently, which is favorable. The light modulation characteristic could not be obtained.
発明の目的 本発明は以上に述べた従来の構造の装荷型方向性結合器
の抱える問題点を克服し、良好な光変調特性を有する方
向性結合器を提供することを目的とする。SUMMARY OF THE INVENTION It is an object of the present invention to provide a directional coupler having good optical modulation characteristics by overcoming the problems of the conventional loaded directional coupler having the above structure.
発明の構成 本発明は従来の構造の装荷型方向結合器において、n型
で低キャリア濃度である光導波層とp型で高キャリア濃
度である第2装荷クラッド層の間に、n型で低キャリア
濃度である第1装荷クラッド層を導入した構造の装荷型
方向性結合器であり、この層の導入によって、第2装荷
クラッド層中のp型不純物が光導波層へ拡散するのを防
止し、また第1装荷クラッド層と光導波層との選択エッ
チングのみで導波路の形状をくずすことなく個々の導波
路を電気的に分離形成でき、良好な光変調特性を得るこ
とができるものである。According to the present invention, in a conventional loaded directional coupler, an n-type and low carrier concentration is provided between an n-type and low carrier concentration optical waveguide layer and a p-type and high carrier concentration second loaded cladding layer. This is a loading type directional coupler having a structure in which a first loading clad layer having a carrier concentration is introduced. By introducing this layer, it is possible to prevent p-type impurities in the second loading clad layer from diffusing into the optical waveguide layer. Further, the individual waveguides can be electrically separated and formed without destroying the shape of the waveguides only by selective etching of the first loading clad layer and the optical waveguide layer, and good optical modulation characteristics can be obtained. .
実施例の説明 第2図は本発明の装荷型方向性結合器の構造を示す断面
図である。ここで1〜6は第1図に示す通りであり、1
0,10′は本発明にかかわる装荷n-−InPクラッド層であ
る。各層のキャリア密度はSドープn+−InP基板1は3
×1018/cm3,Teドープn+−InPバッファー層2は3×1018
/cm3,ノンドープn-−InGaAsP層3は1×1016/cm3,ノン
ドープn-−InPクラッド層10,10′は1×1016/cm3,Znド
ープP+−InP層4,4′は8×1017/cm3である。Description of Embodiments FIG. 2 is a sectional view showing the structure of a loading type directional coupler of the present invention. Here, 1 to 6 are as shown in FIG.
Reference numerals 0 and 10 'are the loaded n -- InP cladding layers according to the present invention. The carrier density of each layer is 3 for S-doped n + -InP substrate 1.
× 10 18 / cm 3 , Te-doped n + -InP buffer layer 2 is 3 × 10 18
/ cm 3, an undoped n - -InGaAsP layer 3 is 1 × 10 16 / cm 3, an undoped n - -InP cladding layer 10, 10 '1 × 10 16 / cm 3, Zn-doped P + -InP layer 4 and 4 ′ Is 8 × 10 17 / cm 3 .
この素子は多層エピタキシャル成長ののち、表面にAu/Z
n電極5,5′,裏面にAu/Sn電極6を蒸着し、表面にフォ
トリソグラフィーにより導波路となるストライプ状のパ
ターンを形成してAu/Zn電極4,4′以外の部分をエッチン
グし、引き続きHCl系のエッチャントによって装荷InPク
ラッド層4,4′,10,10′以外の部分のInP層を選択エッチ
ングによって取り除き、入射端11,出射端12をへき開に
よって形成することによって作製できる。実際にこのよ
うにして作成した素子のAu/Zn電極5,または5′Au/Sn電
極6間に逆バイアスを印加した時、耐圧20V以上、10V印
加した時のリーク電流は1μA以下であった。さらに2
つのAu/Zn電極5,5′間も20V以上の耐圧を示し電気的に
独立であった。This device was grown epitaxially and then Au / Z was formed on the surface.
n / electrodes 5 and 5 ', Au / Sn electrode 6 is vapor-deposited on the back surface, a stripe pattern is formed on the front surface by photolithography, and parts other than the Au / Zn electrodes 4 and 4'are etched. Subsequently, the HCl-based etchant is used to remove the InP layer other than the loaded InP cladding layers 4, 4 ', 10, 10' by selective etching, and the incident end 11 and the outgoing end 12 are formed by cleavage. Actually, when a reverse bias was applied between the Au / Zn electrode 5 and the 5'Au / Sn electrode 6 of the device thus manufactured, the leak current was 1 μA or less when the breakdown voltage was 20 V or more and 10 V was applied. . 2 more
The two Au / Zn electrodes 5 and 5 ′ also showed a withstand voltage of 20 V or more and were electrically independent.
この構造の装荷型方向性結合器の光変調特性を第3図に
示す。ここで横軸は、Au/Zn電極 Au/Sn電極6間に印加
した逆方向電圧であり、縦軸は各導波路端での出射光9,
9′の相対光出力P1,P2である。The optical modulation characteristics of the loaded directional coupler of this structure are shown in FIG. Here, the horizontal axis is the reverse voltage applied between the Au / Zn electrode Au / Sn electrode 6, and the vertical axis is the emitted light at each waveguide end 9,
9'relative light output P 1 , P 2 .
この素子の構造パラメーターとしてT=1.0μmH1=0.3
μm H2=1.0μm W=3.0μm S=3.0μm L=2mmである。
第3図から印加電圧24Vで消光比が20dB程度得られ良好
な光変調特性が得られていることがわかる。As a structural parameter of this device, T = 1.0 μmH 1 = 0.3
μm H 2 = 1.0 μm W = 3.0 μm S = 3.0 μm L = 2 mm.
It can be seen from FIG. 3 that an extinction ratio of about 20 dB is obtained with an applied voltage of 24 V and good optical modulation characteristics are obtained.
以上のように本実施例によれば、装荷型方向性結合器の
n-−InGaAsP光導波層とP+InPクラッド層の間にn-−InP
層を導入することにより、InPの選択エッチングを行な
うだけで電気的に分離できた一対の装荷型導波路が形成
でき、この構造の素子で良好な光変調特性が得られるこ
とができる。なお、本実施例ではInP系材料に限定した
が、光導波層とクラッド層間の選択エッチングが利用で
きるものであればこれらに限られるものではない。As described above, according to this embodiment, the loading type directional coupler
n - n between -InGaAsP optical waveguide layer and the P + InP cladding layer - -InP
By introducing the layer, a pair of loaded waveguides that can be electrically separated can be formed only by performing selective etching of InP, and an excellent optical modulation characteristic can be obtained by the element of this structure. In this embodiment, the material is limited to the InP-based material, but the material is not limited to these as long as the selective etching between the optical waveguide layer and the cladding layer can be used.
発明の効果 本発明の装荷型方向性結合器は、低キャリア濃度でn型
の光導波層と高キャリア濃度でp型の第2装荷クラッド
層の間に、低キャリア濃度でn型の第1装荷クラッド層
を施けることにより、第2装荷クラッド層中のp型不純
物が光導波層へ拡散するのを防止し、また第1装荷クラ
ッド層と光導波層との選択エッチングのみで電気的に分
離された一対の装荷型導波路が形成でき、この素子を用
いれば良好な光変調特性を得ることができ、その実用的
効果は大きい。EFFECTS OF THE INVENTION The loaded directional coupler according to the present invention is provided between the n-type optical waveguide layer having a low carrier concentration and the p-type second loading clad layer having a high carrier concentration, and the first n-type carrier having a low carrier concentration. By providing the loading clad layer, it is possible to prevent p-type impurities in the second loading clad layer from diffusing into the optical waveguide layer, and to electrically perform only by selective etching of the first loading clad layer and the optical waveguide layer. A pair of loaded waveguides separated from each other can be formed, and good optical modulation characteristics can be obtained by using this element, and its practical effect is great.
第1図は従来の装荷型方向性結合器の構造図、第2図は
本発明の一実施例における装荷型方向性結合器の構造
図、第3図は実施例における装荷型方向性結合器の光変
調特性図である。 1……n+−InP基板、2……InPバッファー層、3……n-
InGaAsP層、4,4′……P+InP層、10,10′……n-InPクラ
ッド層。FIG. 1 is a structural diagram of a conventional loading type directional coupler, FIG. 2 is a structural diagram of a loading type directional coupler in an embodiment of the present invention, and FIG. 3 is a loading type directional coupler in an embodiment. It is a light modulation characteristic view of. 1 …… n + −InP substrate, 2 …… InP buffer layer, 3 …… n −
InGaAsP layer, 4,4 '... P + InP layer, 10,10' ... n - InP clad layer.
Claims (1)
波層と、 前記光導波層上に、前記光導波層と選択エッチングでき
る組成であり、n型、低キャリア濃度で所定の幅をも
ち、かつ相互いに平行して形成された一対のストライプ
状第1装荷クラッド層と、 前記第1装荷クラッド層上にこの層とほぼ同じ幅で形成
されたp型で、高キャリア濃度の一対のストライプ状第
2装荷クラッド層と、 前記第2装荷クラッド層上に形成された電極とを備え、 前記第1装荷クラッド層は、前記第2装荷クラッド層か
ら前記光導波層へp型不純物が拡散しないようしてお
り、 前記第1,第2装荷クラッド層は一対のストライプを構成
しており、 前記第1,第2装荷クラッド層により、それぞれの前記ス
トライプ直下の前記光導波層にはそれぞれ光導波路が形
成され、 さらに前記一対のストライプは、それぞれの前記光導波
路を導波する光が結合できる程度に近接して位置し、 前記電極に電圧をかけて前記光導波路にそれぞれ独立し
て逆バイアスを印加することにより、それぞれの前記光
導波路の屈折率を独立に変化させて、前記光導波路から
の出射光を変調することを特徴とする装荷型方向性結合
器。1. An n-type semiconductor substrate, an n-type optical waveguide layer formed on the substrate and having a low carrier concentration, and a composition capable of being selectively etched on the optical waveguide layer with the optical waveguide layer. A pair of striped first loading clad layers having a low carrier concentration and a predetermined width and being parallel to each other; and a p layer formed on the first loading clad layer with a width substantially equal to that of the first loading clad layer. A pair of striped second loading clad layers having a high carrier concentration and an electrode formed on the second loading clad layer, wherein the first loading clad layer comprises the second loading clad layer and the second loading clad layer. The p-type impurities are prevented from diffusing into the optical waveguide layer, and the first and second loading clad layers form a pair of stripes. The first and second loading clad layers directly under the stripes. Of the optical waveguide An optical waveguide is formed on each of the optical waveguides, and the pair of stripes are located close to each other so that light guided through the optical waveguides can be coupled to each other. Then, by applying a reverse bias, the refractive index of each of the optical waveguides is independently changed, and the light emitted from the optical waveguides is modulated.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59069342A JPH0697315B2 (en) | 1984-04-06 | 1984-04-06 | Loaded directional coupler |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59069342A JPH0697315B2 (en) | 1984-04-06 | 1984-04-06 | Loaded directional coupler |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60212727A JPS60212727A (en) | 1985-10-25 |
| JPH0697315B2 true JPH0697315B2 (en) | 1994-11-30 |
Family
ID=13399775
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59069342A Expired - Fee Related JPH0697315B2 (en) | 1984-04-06 | 1984-04-06 | Loaded directional coupler |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0697315B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR20130141850A (en) * | 2012-06-18 | 2013-12-27 | 광주과학기술원 | Optical device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5245296A (en) * | 1975-10-07 | 1977-04-09 | Nippon Telegr & Teleph Corp <Ntt> | Semiconductive phototransmission pass and semiconductor emission devic e used it |
-
1984
- 1984-04-06 JP JP59069342A patent/JPH0697315B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60212727A (en) | 1985-10-25 |
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| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |