JPS6020593A - Manufacture of compound semiconductor element - Google Patents

Manufacture of compound semiconductor element

Info

Publication number
JPS6020593A
JPS6020593A JP12767883A JP12767883A JPS6020593A JP S6020593 A JPS6020593 A JP S6020593A JP 12767883 A JP12767883 A JP 12767883A JP 12767883 A JP12767883 A JP 12767883A JP S6020593 A JPS6020593 A JP S6020593A
Authority
JP
Japan
Prior art keywords
mesa
growth
compound semiconductor
manufacture
semiconductor element
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
Application number
JP12767883A
Other languages
Japanese (ja)
Inventor
Yasutoshi Kashiwada
柏田 泰利
Yoshihisa Fujisaki
芳久 藤崎
Takao Mori
孝夫 森
Yoshinori Nakayama
義則 中山
Shinji Tsuji
伸二 辻
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP12767883A priority Critical patent/JPS6020593A/en
Publication of JPS6020593A publication Critical patent/JPS6020593A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
    • H01S5/22Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers having a ridge or stripe structure
    • H01S5/227Buried mesa structure ; Striped active layer
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
    • H01S5/22Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers having a ridge or stripe structure
    • H01S5/227Buried mesa structure ; Striped active layer
    • H01S5/2275Buried mesa structure ; Striped active layer mesa created by etching

Landscapes

  • Physics & Mathematics (AREA)
  • Geometry (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は化合物半導体素子の製造方法に関する。[Detailed description of the invention] [Field of application of the invention] The present invention relates to a method for manufacturing a compound semiconductor device.

〔発明の背景〕[Background of the invention]

埋込みへテロ構造の半導体素子、たとえば第1図、第2
図に示すGaAtAs系によびInGaAsP系のB 
I−1(Buried−)1eterOstructu
re )型半導体レーザ素子の構造は、一般にメサ部上
端の高さよりその周囲の層の高さの方が相対的に商い構
造を有していた。例えば、M、 Hirao etal
、、 J。
Semiconductor elements with buried heterostructures, for example, FIGS. 1 and 2
B of the GaAtAs and InGaAsP systems shown in the figure.
I-1 (Buried-) 1eter Structure
The structure of the re ) type semiconductor laser device generally has a structure in which the height of the layer around the mesa portion is relatively higher than the height of the upper end of the mesa portion. For example, M. Hirao et al.
,,J.

Appl、Phys、 51 、4539.1980を
参照。ところが近年、結晶と゛成極の接触抵抗の低減な
どの理由により、第1図、第2図に示す構造を作製した
後に、GaAtAs 系の場合のメサ最上Jf4 G 
aAtA sの衣面離化層のエツチングとGaAs1面
層の結晶成長を連続的に行な、う工程や、InGaAs
P系の場合のメサ直上の酸化マスク除去後の新たなIn
GaAsP 表面層の形成工程を採用することにより、
より高信頼度の素子を指向するようになった。ところが
、第1図、第2図に示すようなメサ最上部の高さが周辺
部の高さより相対的に低い状態から出発する従来の素子
作製方法で得た表面層は第3図に示すごとく、液相エピ
タキシャル成長の基本原理上回避できないgraft 
なる結晶欠陥17や溝状を呈するメサ上の成長に起因す
る凹状の未成長部となる欠陥18が発生して、素子の作
製歩留り、信頼性の上で問題が生じていた。
See Appl, Phys, 51, 4539.1980. However, in recent years, for reasons such as reducing the contact resistance between the crystal and the polarization, after fabricating the structure shown in Figs. 1 and 2, the top mesa Jf4 G
InGaAs
New In after removing the oxidation mask directly above the mesa in the case of P-based
By adopting the GaAsP surface layer formation process,
The trend is toward more highly reliable devices. However, the surface layer obtained by the conventional device fabrication method, which starts from a state where the height of the top of the mesa is relatively lower than the height of the surrounding area as shown in Figures 1 and 2, is as shown in Figure 3. , graft cannot be avoided due to the basic principle of liquid phase epitaxial growth.
Crystal defects 17 and defects 18 that are concave ungrown portions caused by growth on the groove-shaped mesa occur, causing problems in the manufacturing yield and reliability of devices.

〔発明の目的〕[Purpose of the invention]

本発明の目的は上記結晶欠陥がメサ上に発生しない作製
方法および素子構造をもって、高歩留り素子作製方法お
よび高信頼素子を提供することにある。
An object of the present invention is to provide a high-yield device fabrication method and a highly reliable device using a fabrication method and device structure in which the above-mentioned crystal defects do not occur on the mesa.

〔発明の概要〕[Summary of the invention]

上記結晶欠陥は、溝状を呈するメサ上の成長に起因する
ことから、メサ直上の成長層形成を伴なう成長を、メサ
表面の旨さがその周囲の結晶表面より相対的に高いか、
すくなくとも同等の形状をもって開始することで問題の
解決を図った。
Since the crystal defects described above are caused by growth on mesas exhibiting a groove shape, growth accompanied by the formation of a growth layer directly above the mesa is determined by whether the quality of the mesa surface is relatively higher than that of the surrounding crystal surfaces.
The problem was solved by starting with at least an equivalent shape.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明の一実施例を第4図により説明する。光通
信用光源として最適なInQaAsP 系の発振波長1
.3μm帯BH型半導体レーザ素子の作製に当シ、先ず
、n〜InP基板結晶19に通常の液相成長によシ20
〜23の4層を多層成長し、5iQ2膜28をマスクと
して設けて湿式化学エツチングにより、20〜23の層
より成るメサを形成した。しかる後、埋込み成長により
層24〜26を得た。但し、層26の表面の高さは層2
3の表面の高さより相対的に低い状態で埋込み成長を完
了した。次に、酸化マスク28を除去して、コンタクト
層27を液相成長により得た。なお、該コンタクト層2
7はキャップ層23よりバンド・ギャップ・エネルギー
Egが小さいInGaAsP組成であって、その後の素
子作製工程で設けるアノード電極との接触抵抗の低下が
可能な層であるが、該メサ形成に用いるエツチング液に
対する性質上、キャップ層23の位置に設けることので
きないノーである。結晶成長後の素子作製工程は従来通
りのため省略する。
An embodiment of the present invention will be described below with reference to FIG. Optimal oscillation wavelength of InQaAsP as a light source for optical communication1
.. To fabricate a 3 μm band BH type semiconductor laser device, first, an n-InP substrate crystal 19 is grown by normal liquid phase growth 20.
A mesa consisting of 20 to 23 layers was formed by growing 4 layers of 20 to 23 layers and performing wet chemical etching using the 5iQ2 film 28 as a mask. Thereafter, layers 24 to 26 were obtained by buried growth. However, the height of the surface of layer 26 is
The buried growth was completed in a state where the height was relatively lower than that of the surface of No. 3. Next, the oxide mask 28 was removed and a contact layer 27 was obtained by liquid phase growth. Note that the contact layer 2
7 is an InGaAsP composition having a smaller band gap energy Eg than the cap layer 23, and is a layer that can reduce the contact resistance with the anode electrode provided in the subsequent device fabrication process. Due to its nature, it cannot be provided at the position of the cap layer 23. The device fabrication process after crystal growth is the same as before and will be omitted.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、素子の注入電流−光出力特性、長期寿
命特性に悪影響を及ぼす結晶欠陥17゜18のうち、1
7は従来の100チ発生から皆無に、18は従来の20
0〜1300ケ/Crn2から皆無にすることができ、
素子の作製歩留り向上と高信頼度化に効果がある。
According to the present invention, 1 out of 17°18 crystal defects that adversely affect the injection current-optical output characteristics and long-term life characteristics of the device
7 has been completely eliminated from the conventional 100-chi occurrence, and 18 has been reduced from the conventional 20-chi.
It can be completely eliminated from 0 to 1300 cases/Crn2,
This is effective in improving device manufacturing yield and increasing reliability.

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

第1図、第2図は従来のBH型半導体レーザ素子の、レ
ーザ光出射方向からの断面図、第3図は第1図、第2図
の構造を有する結晶上にさらに成長層を設けた素子のレ
ーザ光出射方向からの断面図、第4図は本発明のBH型
半導体レーザ素子のレーザ光出射方向からの断面図。
Figures 1 and 2 are cross-sectional views of a conventional BH-type semiconductor laser device taken from the laser beam emission direction, and Figure 3 shows a crystal with the structure shown in Figures 1 and 2 further provided with a growth layer. FIG. 4 is a sectional view of the BH type semiconductor laser device of the present invention taken from the laser beam emission direction.

Claims (1)

【特許請求の範囲】[Claims] 1、連台形のメサを有する埋込みへテロ構造の半導体素
子の結晶成長工程において、メサ直上への成長層形成を
伴なう成長を、メサ直上の結晶表面高さが周囲の結晶表
面高さより相対的に高いかあるいは同等の形状をもって
開始することを特徴とする化合物半導体素子の製造方法
1. In the crystal growth process of a semiconductor device with a buried heterostructure having a series of trapezoidal mesas, the crystal surface height directly above the mesa is relative to the surrounding crystal surface height. 1. A method for manufacturing a compound semiconductor device, characterized in that the method starts with a shape that is higher than or equal to the shape of the semiconductor device.
JP12767883A 1983-07-15 1983-07-15 Manufacture of compound semiconductor element Pending JPS6020593A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12767883A JPS6020593A (en) 1983-07-15 1983-07-15 Manufacture of compound semiconductor element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12767883A JPS6020593A (en) 1983-07-15 1983-07-15 Manufacture of compound semiconductor element

Publications (1)

Publication Number Publication Date
JPS6020593A true JPS6020593A (en) 1985-02-01

Family

ID=14965998

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12767883A Pending JPS6020593A (en) 1983-07-15 1983-07-15 Manufacture of compound semiconductor element

Country Status (1)

Country Link
JP (1) JPS6020593A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5721751A (en) * 1993-10-28 1998-02-24 Nippon Telegraph & Telephone Corporation Semiconductor laser

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5721751A (en) * 1993-10-28 1998-02-24 Nippon Telegraph & Telephone Corporation Semiconductor laser

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