JPS63216396A - Semiconductor light emitting devices - Google Patents
Semiconductor light emitting devicesInfo
- Publication number
- JPS63216396A JPS63216396A JP5072487A JP5072487A JPS63216396A JP S63216396 A JPS63216396 A JP S63216396A JP 5072487 A JP5072487 A JP 5072487A JP 5072487 A JP5072487 A JP 5072487A JP S63216396 A JPS63216396 A JP S63216396A
- Authority
- JP
- Japan
- Prior art keywords
- light emitting
- active layer
- etching
- layer
- semiconductor light
- 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.)
- Pending
Links
- 239000004065 semiconductor Substances 0.000 title claims abstract description 15
- 238000005530 etching Methods 0.000 claims abstract description 13
- 230000010355 oscillation Effects 0.000 claims abstract description 5
- 230000005284 excitation Effects 0.000 claims 1
- 239000013078 crystal Substances 0.000 abstract description 22
- 238000001312 dry etching Methods 0.000 abstract description 6
- 239000000463 material Substances 0.000 abstract description 6
- 239000000758 substrate Substances 0.000 abstract description 5
- 230000000694 effects Effects 0.000 abstract description 4
- 238000010438 heat treatment Methods 0.000 abstract description 2
- GWEVSGVZZGPLCZ-UHFFFAOYSA-N Titan oxide Chemical compound O=[Ti]=O GWEVSGVZZGPLCZ-UHFFFAOYSA-N 0.000 abstract 2
- 238000005253 cladding Methods 0.000 description 11
- 238000000034 method Methods 0.000 description 6
- 230000003287 optical effect Effects 0.000 description 5
- 238000005520 cutting process Methods 0.000 description 2
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 description 1
- 240000002329 Inga feuillei Species 0.000 description 1
- 230000004075 alteration Effects 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000003486 chemical etching Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000005281 excited state Effects 0.000 description 1
- 239000012467 final product Substances 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 238000009499 grossing Methods 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 230000002250 progressing effect Effects 0.000 description 1
- 238000007790 scraping Methods 0.000 description 1
- 238000001179 sorption measurement Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明はエツチングにより共振器端面を削り出して作製
する半導体発光素子に関し、特に信頼性を高めた半導体
発光素子を提供するものでおる。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a semiconductor light emitting device manufactured by cutting out a resonator end face by etching, and particularly provides a semiconductor light emitting device with improved reliability.
(従来の技術〕
近年光通信や光情報分野の発展には著しいものがあり、
それらの実用化は急速に進展してい′る。こうした中で
信号の媒体であるレーザーの光源としては指向性や単色
性に優れた半導体発光素子が不可欠なものとなっている
。(Conventional technology) In recent years, there has been remarkable development in the fields of optical communication and optical information.
Their practical application is progressing rapidly. Under these circumstances, semiconductor light emitting devices with excellent directivity and monochromaticity have become indispensable as light sources for lasers, which are signal media.
上記半導体発光素子(以下単に発光素子と記す)を作製
する際に、該素子のレーザー共振器端面、即ち発光素子
内で発生するレーザーの反射面であって、レーザーの出
力方向に直交する面を形成する時には通常は結晶の襞間
面をそのまま共振器端面(以下反射面と記す)として用
いている。しかも襞間という単純な操作で得られるため
、盛んに利用されている。When manufacturing the above-mentioned semiconductor light emitting device (hereinafter simply referred to as a light emitting device), the laser resonator end face of the device, that is, the surface that reflects the laser generated within the light emitting device and is perpendicular to the output direction of the laser, is During formation, the interfold surfaces of the crystal are usually used as they are as resonator end surfaces (hereinafter referred to as reflective surfaces). Moreover, it is widely used because it can be obtained by a simple operation of interfolding.
この襞間面を反射面として利用する発光素子は該素子を
単体で用いる限りは何ら問題はない。There is no problem with a light emitting element that utilizes the interfold surface as a reflective surface as long as the element is used alone.
しかし、上記襞間面では結晶が断絶しているため、この
ような発光素子にディテクターや駆動用回路等信の光機
能デバイスを一体に集積させることはできない。従って
発光素子を基にして光集積回路や光集積デバイスを構成
するには襞間以外の方法でレーザー反射面をつくる必要
がある。However, since the crystal is discontinued at the interfold plane, optical functional devices such as a detector and a driving circuit cannot be integrated into such a light emitting element. Therefore, in order to construct an optical integrated circuit or optical integrated device based on a light emitting element, it is necessary to create a laser reflecting surface by a method other than between the folds.
これに対処するために、従来から襞間面でない面をエツ
チングにより平坦に削り出して反射面とする方法が行な
われている。一般的なエツチングの方法には化学反応を
利用する化学エツチングと励起状態の分子、原子又はイ
オン等の低温プラズマを利用するドライエツチングとが
あるが、化学エツチングはエツチング速度が結晶面の方
向や結晶の種類により異なってしまい、このままでは反
射面として使うのには不適当である。一方ドライエツチ
ングはエツチングの選択性が小さく歩留り及び再現性に
優れ、良好な微細加工性を有するため、集積化に最も適
した反射面の形成方法である。In order to cope with this problem, a method has conventionally been used in which a surface that is not an interfold surface is cut flat by etching to form a reflective surface. General etching methods include chemical etching, which uses chemical reactions, and dry etching, which uses low-temperature plasma of molecules, atoms, or ions in an excited state. This varies depending on the type of surface, and as it is, it is unsuitable for use as a reflective surface. On the other hand, dry etching has low etching selectivity, excellent yield and reproducibility, and good microfabrication, so it is the most suitable method for forming reflective surfaces for integration.
発光素子にはInP系や(3aAs系があり、その構造
は異なった種類で格子定数の等しい半導体結晶同士を同
じ結晶方位で接合させたヘテロ接合が2箇所存在するダ
ブルへテロ構造が一般的である。例えばInP系ではI
nP単結晶基板上にInP単結晶のクラッド層を成長さ
せ、その上にInGaAsP単結晶の活性層及びInP
単結晶のクラッド層を順に成長させた多層構造となって
いる。このように積層した結晶を襞間等の方法により切
り出し、電極を形成して発光素子とする。該素子に電圧
を印加することにより、各単結晶の積層方向と直交する
方向にレーザーが発せられる。Light-emitting devices include InP-based and (3aAs-based), and their structure generally has a double heterostructure in which there are two heterojunctions in which semiconductor crystals of different types with the same lattice constant are joined in the same crystal orientation. For example, in InP system, I
An InP single crystal cladding layer is grown on an nP single crystal substrate, and an InGaAsP single crystal active layer and an InP single crystal cladding layer are grown on top of the InP single crystal cladding layer.
It has a multilayer structure in which single-crystal cladding layers are grown in sequence. The thus laminated crystals are cut out by a method such as interfolding, and electrodes are formed to form a light emitting element. By applying a voltage to the element, a laser is emitted in a direction perpendicular to the stacking direction of each single crystal.
(発明が解決しようとする問題点)
ドライエツチングによりレーザーの反射面を形成して、
発光素子を作製した場合、該反射面はドライエツチング
の実施中に低温プラズマにより過度の物理的ダメージを
受けたり使用雰囲気中の酸素、水分又は他の不純物の吸
着により化学的変質を受けたりする。一方発光素子を構
成する活性層はレーザー発振を行なっている部位である
が反射面に露出する活性層が上記のような損傷を受けた
場合はレーザーの発振状態の不安定性が増大し、寿命が
短くなる等信頼性の低下が問題となっていた。(Problem to be solved by the invention) A laser reflective surface is formed by dry etching,
When a light emitting device is fabricated, the reflective surface may be subjected to excessive physical damage due to low temperature plasma during dry etching or chemical alteration due to adsorption of oxygen, moisture or other impurities in the operating atmosphere. On the other hand, the active layer that makes up the light emitting device is the part that performs laser oscillation, but if the active layer exposed to the reflective surface is damaged as described above, the instability of the laser oscillation state will increase and the lifespan will be shortened. There was a problem of decreased reliability due to shorter lengths.
本発明はこれに鑑み種々検討の結果、信頼性の高い半導
体発光素子を開発したもので、エツチングにより反射面
を対向して形成する発光素子において、該反射面内側に
非励起領域を設けることを特徴とするものである。In view of this, as a result of various studies, the present invention has developed a highly reliable semiconductor light emitting device.In a light emitting device in which reflective surfaces are formed facing each other by etching, a non-excited region is provided inside the reflective surfaces. This is a characteristic feature.
(作 用)
上記のような非励起領域を形成するには、エツチングに
よりレーザーの反射面を削り出す時に又は該反射面を削
り出した後に活性層だけを選択エツチングによりわずか
に深くエツチングして凹状の溝を形成させ、しかる後質
量輸送法により該溝を挟んで両側に突出したクラッド層
から結晶を構成する原子を凹状の溝に輸送し、クラッド
層と同じ結晶を形成させ、表面の凹凸をなくして新たな
反射面とすればよい。(Function) In order to form the above-mentioned non-excited region, when or after cutting out the laser reflecting surface by etching, only the active layer is selectively etched slightly deeper to create a concave shape. After that, the atoms constituting the crystal are transported from the cladding layer protruding on both sides of the groove to the concave groove using the mass transport method, forming the same crystal as the cladding layer, and smoothing out the surface irregularities. It can be removed and used as a new reflective surface.
(実施例)
本発明の一実施例としてレーザー波長1.3μmのI
rlGaAs P/ I rl P半導体発光素子を第
1図(イ)、(ロ)、(ハ)に示す。先ず第1図(イ)
に示すようにn型−InP単結晶基板(1)上に該基板
(1)と同じ結晶方位でn型−InP単結晶クラッド層
(2)を成長させ、該クラッド層(2)の上にInGa
ASP単結晶活性層(3)をヘテロ接合を形成するよう
に結晶成長させ、ざらに該活性層(3)の上にp型−I
nP単結晶クラッド層(4) 、 p型−GaInAs
Pキャップ層(4゛)を同じくヘテロ接合を形成するよ
うに結晶成長させた後、該キャップ層(4°)表面にT
i0z膜をエツチングのマスク材(5)として施し、そ
の後該マスク材(5)のエツチングパターンによりマス
ク材(5)の形成面をエツチングにより削り出した。し
かるi多層 12−Arガスによる低温プラズマを用い
たドライエツチングにより反射面(6)、 (7)を各
層の方向と直交する方向で襞間面以外の対向する面に形
成した。(Example) As an example of the present invention, I
An rlGaAs P/IrlP semiconductor light emitting device is shown in FIGS. 1(a), (b), and (c). First, Figure 1 (a)
As shown in the figure, an n-type InP single crystal cladding layer (2) is grown on an n-type InP single crystal substrate (1) in the same crystal orientation as the substrate (1), and on top of the cladding layer (2). InGa
The ASP single crystal active layer (3) is crystal-grown to form a heterojunction, and the p-type -I layer is roughly grown on the active layer (3).
nP single crystal cladding layer (4), p-type-GaInAs
After crystal-growing a P cap layer (4°) to form a heterojunction, T
The i0z film was applied as an etching mask material (5), and then the surface on which the mask material (5) was formed was etched out according to the etching pattern of the mask material (5). Reflective surfaces (6) and (7) were formed on opposing surfaces other than the inter-fold surfaces in a direction perpendicular to the direction of each layer by dry etching using low-temperature plasma using 12-Ar gas.
次に第1図(ロ)に示すように上記反射面(6)、 (
7)に露出している活性層(3)を選択エツチングによ
り、わずかに削り取った後、この半導体結晶(8)をP
H3雰囲気中にて600 ’Cに加熱し、質量輸送現象
により活性層(3)両側のクララド層(2)、 (4)
から1n及びP@選択エツチングされた活性層の溝部に
輸送し、第1図(ハ)に示すようにInP単結晶を形成
して非励起領域(9L(9“)を設け、端面、即ち反射
面(6)、 (7)を平坦化する。その後マスク材(5
)を除去し、基板(1)側及びその反対側に電極(10
)、 (11)を形成した。Next, as shown in Figure 1 (b), the reflective surface (6), (
After slightly scraping off the active layer (3) exposed in 7) by selective etching, this semiconductor crystal (8) is
Heating to 600'C in H3 atmosphere, mass transport phenomenon creates Clarado layers (2), (4) on both sides of active layer (3).
1n and P@ are transported to the groove of the selectively etched active layer, and as shown in FIG. Planarize surfaces (6) and (7). Then mask material (5)
) is removed, and electrodes (10
), (11) were formed.
このように作製した半導体発光素子のレーザー反射面の
活性層にはレーザー発振に寄与しない非励起領域が形成
されていることが確められlこ。It was confirmed that a non-excited region that does not contribute to laser oscillation was formed in the active layer of the laser reflecting surface of the semiconductor light emitting device fabricated in this way.
このように本発明によれば半導体発光素子にあけるレー
ザー反射面の損傷の影響を除去でき信頼性の高いレーザ
ーを得ることができる等工業上顕著な効果を奏するもの
でおる。As described above, the present invention has industrially significant effects such as being able to eliminate the effects of damage to the laser reflecting surface in the semiconductor light emitting device and producing a highly reliable laser.
第1図(イ)、(ロ)、(ハ)は本発明の一実施例を示
すもので、(イ)は単結晶を層状に成長させた側断面図
、(ロ)は活性層を選択エツチングした状態を示す側断
面図、(ハ)は最終製品を示す側断面図である。
1・・・・・・・・n型InP基板
2・・・・・・・・n型InPクラッド層3・・・・・
・・・I nGaASP活性層4・・・・・・・・p型
1nPクラッド層4°・・・・・・・・p型GaInA
SPキャップ層5・・・・・・・・マスク材
6.7・・・・・・反射面
8・・・・・・・・半導体発光素子
9.9°・・・・・・非励起領域
to、 ii・・・・電極Figures 1 (a), (b), and (c) show one embodiment of the present invention, in which (a) is a side sectional view of a single crystal grown in layers, and (b) is a selected active layer. (C) is a side sectional view showing the etched state, and (c) is a side sectional view showing the final product. 1...N-type InP substrate 2...N-type InP cladding layer 3...
...I nGaASP active layer 4...P-type 1nP cladding layer 4°...P-type GaInA
SP cap layer 5...Mask material 6.7...Reflecting surface 8...Semiconductor light emitting element 9.9°...Non-excitation region to, ii...electrode
Claims (1)
発光素子において、該共振器端面内側に非励起領域或い
はレーザの発振波長に対し透明となる窓領域を設けるこ
とを特徴とする半導体発光素子。1. A semiconductor light emitting device in which resonator end faces are formed by etching to face each other, and the semiconductor light emitting device is characterized in that a non-excitation region or a window region transparent to the oscillation wavelength of a laser is provided inside the resonator end face.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5072487A JPS63216396A (en) | 1987-03-05 | 1987-03-05 | Semiconductor light emitting devices |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5072487A JPS63216396A (en) | 1987-03-05 | 1987-03-05 | Semiconductor light emitting devices |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63216396A true JPS63216396A (en) | 1988-09-08 |
Family
ID=12866814
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5072487A Pending JPS63216396A (en) | 1987-03-05 | 1987-03-05 | Semiconductor light emitting devices |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63216396A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5608750A (en) * | 1993-07-29 | 1997-03-04 | Hitachi, Ltd. | Semiconductor laser device and a method for the manufacture thereof |
JP2013191622A (en) * | 2012-03-12 | 2013-09-26 | Mitsubishi Electric Corp | Semiconductor light-emitting element and manufacturing method of the same |
-
1987
- 1987-03-05 JP JP5072487A patent/JPS63216396A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5608750A (en) * | 1993-07-29 | 1997-03-04 | Hitachi, Ltd. | Semiconductor laser device and a method for the manufacture thereof |
JP2013191622A (en) * | 2012-03-12 | 2013-09-26 | Mitsubishi Electric Corp | Semiconductor light-emitting element and manufacturing method of the same |
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