JPS5875877A - Monitor built-in semiconductor laser element - Google Patents

Monitor built-in semiconductor laser element

Info

Publication number
JPS5875877A
JPS5875877A JP56174107A JP17410781A JPS5875877A JP S5875877 A JPS5875877 A JP S5875877A JP 56174107 A JP56174107 A JP 56174107A JP 17410781 A JP17410781 A JP 17410781A JP S5875877 A JPS5875877 A JP S5875877A
Authority
JP
Japan
Prior art keywords
region
current injection
electrode
monitor
type
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
JP56174107A
Other languages
Japanese (ja)
Other versions
JPS6320396B2 (en
Inventor
Hidenori Nomura
野村 秀徳
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP56174107A priority Critical patent/JPS5875877A/en
Publication of JPS5875877A publication Critical patent/JPS5875877A/en
Publication of JPS6320396B2 publication Critical patent/JPS6320396B2/ja
Granted 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
    • H01S5/02Structural details or components not essential to laser action
    • H01S5/026Monolithically integrated components, e.g. waveguides, monitoring photo-detectors, drivers
    • H01S5/0262Photo-diodes, e.g. transceiver devices, bidirectional devices
    • H01S5/0264Photo-diodes, e.g. transceiver devices, bidirectional devices for monitoring the laser-output
    • 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
    • H01S5/04Processes or apparatus for excitation, e.g. pumping, e.g. by electron beams
    • H01S5/042Electrical excitation ; Circuits therefor
    • H01S5/0421Electrical excitation ; Circuits therefor characterised by the semiconducting contacting layers
    • 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
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/305Structure or shape of the active region; Materials used for the active region characterised by the doping materials used in the laser structure
    • H01S5/3054Structure or shape of the active region; Materials used for the active region characterised by the doping materials used in the laser structure p-doping

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Solid State Image Pick-Up Elements (AREA)
  • Semiconductor Lasers (AREA)

Abstract

PURPOSE:To build-in a high sensitivity monitor without deterioration of laser operating characteristics in a monitor built-in semiconductor laser element by integrating a phototransitor structure containing a base region formed of a collector electrode and a photo-occluding layer isolated from a current injection electrode. CONSTITUTION:This laser is composed of an active region 11 having a buried structure formed on an n type semiconductor substrate 10, a clad region 12 made of a p type semiconductor, a photoabsorbing layer 13 on the region 12, an n type side electrode 19, a current injection electrode 17, and a collector electrode 18. The layer 13 is formed of n type reverse to the region 12 at the time of growing crystal, and a current injection stripe region 15 connected to the regions 14, 12 by thermal diffusion of the p type impurity is contained therein. The electrodes 17, 18 are electrically isolated via an insulating film 16.

Description

【発明の詳細な説明】 本発明は光フアイバ通信用もしくは光情報処理用光源と
して使用される半導体レーザ素子の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in semiconductor laser devices used as light sources for optical fiber communications or optical information processing.

半導体レーザ素子は小型で高い電力効率更に他のレーザ
にはない長寿命と保守の容易さとによって、近年光フア
イバ通信用、あるいは光情報処理用の光源として益々そ
の用途を広めている。しかしながら、半導体レーザは周
囲温度の変化に伴って発振閾値が変化し従って光出力が
変動するという特性を有している。このため従来の半導
体レーザ素子は光出力変動をモニタするフォトダイオー
ドと共に使用し光出力を一定番ζ保つためのバイアス電
流調整回路が付加されていた。フォトダイオードと半導
体レーザ素子をモノリシックに集積化し素子組立の工数
削減と素子全体の小型化を目的としたモニタ内蔵半導体
レーザ素子も知られている。
Semiconductor laser elements have been increasingly used as light sources for optical fiber communications and optical information processing in recent years due to their small size, high power efficiency, long lifespan, and ease of maintenance not found in other lasers. However, semiconductor lasers have the characteristic that their oscillation threshold changes with changes in ambient temperature, and accordingly, their optical output fluctuates. For this reason, conventional semiconductor laser devices are used together with a photodiode to monitor variations in optical output, and a bias current adjustment circuit is added to maintain the optical output at a constant value ζ. A semiconductor laser device with a built-in monitor is also known, which monolithically integrates a photodiode and a semiconductor laser device for the purpose of reducing the number of steps for assembling the device and downsizing the device as a whole.

しかしながら、従来のモニタ内蔵半導体レーザ素子では
レーザの光出力ビーム方向にレーザと縦続する形にモニ
タ用フォトダイオードを形成していた。このため、従来
例では結晶のへき開面に比べれば特性の劣るエツチング
鏡面によってレーザを構成し、レーザとは分離されたフ
ォトダイオードを作っていた。特性の劣る鏡面はレーザ
動作の劣化をもたらし、またレーザ動作部の活性層と共
通化されたフォトダイオードの光吸収部はフォトダイオ
ードの特性を向上させる上での障害になるという欠点を
有していた。
However, in a conventional semiconductor laser device with a built-in monitor, a monitor photodiode is formed to be cascaded with the laser in the optical output beam direction of the laser. For this reason, in the conventional example, a laser was constructed using an etched mirror surface whose characteristics were inferior to that of a cleavage plane of a crystal, and a photodiode separate from the laser was manufactured. A mirror surface with poor characteristics causes deterioration of laser operation, and the photodiode's light absorption section, which is shared with the active layer of the laser operating section, has the disadvantage of becoming an obstacle to improving the photodiode's characteristics. Ta.

本発明の目的は上述の欠点を除去し、高感度なモニタを
内蔵しかつレーザ動作特性の劣化も伴なわないモニタ内
蔵半導体レーザ素子を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks and to provide a semiconductor laser device with a built-in monitor that has a built-in highly sensitive monitor and does not cause deterioration of laser operating characteristics.

本発明によれば、半導体へテロ綱合を含む半導体多層構
造を有して構成される電流注入形牛導体レーザ素子にお
いて、電流注入用電極とは分離されたコレクタ電極及び
光吸収層で形成されたベース領域を含むフォトトランジ
スタ構造が集積化されたことを特徴とするモニタ内蔵半
導体レーザ素子が得られる。
According to the present invention, in a current injection type conductor laser element having a semiconductor multilayer structure including a semiconductor heterostructure, a collector electrode and a light absorption layer are formed, which are separated from a current injection electrode. A semiconductor laser device with a built-in monitor is obtained, which is characterized in that a phototransistor structure including a base region is integrated.

次に図面を参照して本発明の詳細な説明する。Next, the present invention will be described in detail with reference to the drawings.

図面は本発明の一実施例につき、そのレーザ光出力ビー
ム方向と垂直な断面を表わす図である。本実施例はn形
の半導体基板lOの上に形成され埋め込まれた構造を有
する活性領域11とp形半導体から成るクラッド領域1
2とそのクラッド領域12上の光吸収層13及びn側電
極19と電流注入用電極17とコレクタ電極18によっ
て構成されている。光吸収層13は結晶成長時にはクラ
ッド領域11!とは反対導電形のn形で形成されたあと
、p形不純物の熱拡散によるコレクタ領域14及びクラ
ッド領域12へつながる電流注入ストライプ領域1sを
その内部番ζ含んでいる。なお電流注入用電極17とコ
レクタ電極18とは絶縁膜16によって電気的に分離さ
れている。各主要部の組成及び寸法を述べれば、半導体
基板10は面方位(10G)のImP単結晶で厚さ約7
0μm1活性領域11は(010方向に延びたストライ
プ状で幅2pm、厚go、1$fim、発振波長1.3
am に相当するIn&ra Gate−人1&IlP
&44sクラッド領域12は活性領域11上の厚さが約
2μmのZmドープInk、光吸収層13は厚さ約1.
5μm1吸収端波長1115mIc@?AするInty
mGaassA@a・雪Pa5s、電流注入ストライプ
領域1sは深さ約2μmのZn拡散によってp形に反転
されており、活性領域11を中心とする幅約8μm1コ
レクタ領域14は深さ1μmのZn拡散番ζよってp形
に反転され電流注入ストライプ領域1bとは約10μm
の間隔を詔いて設けられた幅約201smのストライプ
状、絶縁膜16は厚$0.24mの一810m  、 
s流注入用電極17とコレクタ電極18は厚さ約0.3
μmのムu−Zn合金、n側電極、19は厚さ約0.3
μmのムu−8n合金である。素子は活性領域11のス
トライプ方向と直角な方向番とへき開によつて切り出さ
れ、その共振器長は約250μmである。
The drawing is a cross-sectional view perpendicular to the laser light output beam direction of one embodiment of the present invention. In this embodiment, an active region 11 having a buried structure formed on an n-type semiconductor substrate IO and a cladding region 1 made of a p-type semiconductor
2, a light absorption layer 13 on the cladding region 12, an n-side electrode 19, a current injection electrode 17, and a collector electrode 18. The light absorbing layer 13 is the cladding region 11 during crystal growth! The current injection stripe region 1s is formed of n-type, which is the opposite conductivity type, and then connected to the collector region 14 and cladding region 12 by thermal diffusion of p-type impurities. Note that the current injection electrode 17 and the collector electrode 18 are electrically separated by an insulating film 16. To describe the composition and dimensions of each main part, the semiconductor substrate 10 is made of an ImP single crystal with a plane orientation (10G) and has a thickness of about 7 mm.
The active region 11 has a width of 2 pm, a thickness of go, 1 $fim, and an oscillation wavelength of 1.3.
In&ra Gate-Person 1&IlP equivalent to am
The &44s cladding region 12 is made of Zm-doped Ink with a thickness of about 2 μm on the active region 11, and the light absorption layer 13 is made of Zm-doped Ink with a thickness of about 1.5 μm.
5μm1 absorption edge wavelength 1115mIc@? Inty to A
mGaassA@a/Snow Pa5s, the current injection stripe region 1s is inverted to p-type by Zn diffusion with a depth of about 2 μm, and the width of the collector region 14 with a width of about 8 μm centered on the active region 11 is Zn diffused with a depth of 1 μm. ζ Therefore, the current injection stripe region 1b, which is inverted to p-type, is about 10 μm.
The insulating film 16 has a stripe shape with a width of about 201 sm provided at intervals of 1810 m with a thickness of $0.24 m,
The s-flow injection electrode 17 and the collector electrode 18 have a thickness of approximately 0.3
μm μm u-Zn alloy, n-side electrode, 19 has a thickness of about 0.3
It is a μm U-8N alloy. The device is cut out by cleavage and a direction perpendicular to the stripe direction of the active region 11, and its resonator length is about 250 μm.

さて、電流注入用電極17に正電圧、n側電極19に負
電圧を印加して、電流注入ストライプ領域1s及びクラ
ッド領域12を通して活性領域11へ電流を注入すると
、電流30〜40mA以上注入した所でレーザ発振を開
始する。コレクタ電極18には負の電圧を印加しておく
。活性領域11とクラッド領域12の界面にaける光学
的不完全性によって散乱されたレーザ光出力の一部はベ
ース領域11mで吸収され光励起電流を発生する。
Now, when a positive voltage is applied to the current injection electrode 17 and a negative voltage is applied to the n-side electrode 19, and a current is injected into the active region 11 through the current injection stripe region 1s and the cladding region 12. Start laser oscillation. A negative voltage is applied to the collector electrode 18 in advance. A portion of the laser light output scattered by the optical imperfection a at the interface between the active region 11 and the cladding region 12 is absorbed by the base region 11m and generates a photoexcitation current.

この光励起電流はクラッド領域12及びベース領域13
鳳及びコレクタ領域14が構成するヘテロ接合pup形
フオ))ランジスタ構造の高い電流増幅車番ζよって増
1されコレクタ電極18から取り出される。フォトダイ
オードを集積化した従来例では、フォトダイオードの光
吸収層がレーザの活性層と同一とすることが多かったた
めに、受光効率が低く、小さなモニタ電流しか得られな
かったのに対して、本実施例では、光吸収層13の組−
成を活性領域11の組成とは無関係に最適化できるので
、高い受光効率が得られ更にフォトトランジスタ構造の
高い増幅率によって増幅されるのでわずかな散乱光を利
用するだけで十分なモニタ電流を得ることができる。ま
た本実施例ではモニタ部がレーザ部と並列されているた
めに、従来の半導体レーザ素子と同じく、結晶のへき開
番こよって共振器を形成できるという利点もある。
This photoexcited current flows through the cladding region 12 and the base region 13.
A high current amplification wheel number ζ of the transistor structure is increased by the heterojunction pup-type photoconductor formed by the collector region 14 and the collector region 14, and is taken out from the collector electrode 18. In conventional integrated photodiodes, the light absorption layer of the photodiode was often the same as the active layer of the laser, resulting in low light reception efficiency and only a small monitor current. In the embodiment, the set of light absorption layers 13-
Since the composition of the active region 11 can be optimized independently of the composition of the active region 11, high light reception efficiency can be obtained, and since it is amplified by the high amplification factor of the phototransistor structure, a sufficient monitor current can be obtained by using only a small amount of scattered light. be able to. Further, in this embodiment, since the monitor section is arranged in parallel with the laser section, there is an advantage that a resonator can be formed by cleaving the crystal, as in the conventional semiconductor laser device.

ところで上述の実施例ではクラッド領域12に電流阻止
構造を有しないものとしたが、n形半導体からなる電流
阻止層を加えても良い。また、電流注入形半導体レーザ
索子の構造に関しても上述の構造には限定されず、他の
壌め込み構造でもよ<、tた活性層が平間的広がりを有
する非理め込み構造でもよい。半導体材料は必ずしもI
nk/lmGaムsr  jl111C限らずGaAs
 / G a A I A s系など半導体レーザ素子
が構成可能な材料ならばいずれでも嵐い。
By the way, in the above embodiment, the cladding region 12 does not have a current blocking structure, but a current blocking layer made of an n-type semiconductor may be added. Furthermore, the structure of the current injection type semiconductor laser beam is not limited to the above-mentioned structure, and may be any other type of embedded structure, or may be a non-embedded structure in which the active layer has a flat width. Semiconductor materials are not necessarily I
nk/lmGamussr jl111C as well as GaAs
Any material that can be used to construct a semiconductor laser device, such as Ga AI A S type, is suitable.

最後iと本発明が有する利点を要約すれば、へき開面利
用の高性能な半導体レーザ素子に高感度なモニタを内蔵
することにより、大出力の安定化にとって便利なモニタ
内蔵半導体レーザ素子が得られることである。
Finally, to summarize the advantages of the present invention, by incorporating a highly sensitive monitor into a high-performance semiconductor laser device that uses cleavage planes, a semiconductor laser device with a built-in monitor that is convenient for stabilizing high output can be obtained. That's true.

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

図画は一5I!施例の断面図である。 図中、 10・・・・・・半導体基板、11−・・・・・活性領
域、12・・・・・・クラッド領域、13・・・・・・
光吸収層、1381・・・ベース領域、14−・・・・
・コレクタ領域、15・・・・・・電流注入ストライプ
領域、16・・・・・・絶縁膜、17・・・・・・電流
注入用電極、18・・・・・・コレクタ電極、′19・
・・・・・n側電極である。
Drawing is 15I! It is a sectional view of an example. In the figure, 10... semiconductor substrate, 11-... active region, 12... cladding region, 13......
Light absorption layer, 1381...Base region, 14-...
- Collector region, 15... Current injection stripe region, 16... Insulating film, 17... Current injection electrode, 18... Collector electrode, '19・
...This is an n-side electrode.

Claims (1)

【特許請求の範囲】 (1)  半導体へテロ接金を含む半導体多層構造を有
して構成される電流注入形牛導体レーザ素子に詔いて、
電流注入用電極とは分離されたコレクタ電極及び光吸収
層で形成されたベース領域を含むフォトトランジスタ構
造が集積化された仁とを特徴とするモニタ内蔵半導体レ
ーザ素子。 (8)前記電流注入形中導体レーザ素子が埋め込み構造
活性領域を有し、かつ前記ベース領域が前記活性領域の
上方から離れた位置番ζ設けられていることを特徴とす
る特許請求の範囲第1項記載のモニタ内蔵半導体レーザ
素子。
[Scope of Claims] (1) A current injection type conductor laser element configured with a semiconductor multilayer structure including semiconductor heterojunction,
A semiconductor laser device with a built-in monitor, characterized in that a phototransistor structure including a collector electrode separated from a current injection electrode and a base region formed of a light absorption layer is integrated. (8) The current injection type medium conductor laser element has a buried structure active region, and the base region is provided at a position ζ apart from above the active region. The semiconductor laser device with a built-in monitor according to item 1.
JP56174107A 1981-10-30 1981-10-30 Monitor built-in semiconductor laser element Granted JPS5875877A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56174107A JPS5875877A (en) 1981-10-30 1981-10-30 Monitor built-in semiconductor laser element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56174107A JPS5875877A (en) 1981-10-30 1981-10-30 Monitor built-in semiconductor laser element

Publications (2)

Publication Number Publication Date
JPS5875877A true JPS5875877A (en) 1983-05-07
JPS6320396B2 JPS6320396B2 (en) 1988-04-27

Family

ID=15972765

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56174107A Granted JPS5875877A (en) 1981-10-30 1981-10-30 Monitor built-in semiconductor laser element

Country Status (1)

Country Link
JP (1) JPS5875877A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4674100A (en) * 1983-10-06 1987-06-16 Nec Corporation Bistable optical device
FR2592239A1 (en) * 1985-12-25 1987-06-26 Kokusai Denshin Denwa Co Ltd SEMICONDUCTOR LASER WITH DISTRIBUTED FEEDBACK WITH MONITOR.

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5214393A (en) * 1975-07-16 1977-02-03 Post Office Laser and optical detector

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5214393A (en) * 1975-07-16 1977-02-03 Post Office Laser and optical detector

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4674100A (en) * 1983-10-06 1987-06-16 Nec Corporation Bistable optical device
FR2592239A1 (en) * 1985-12-25 1987-06-26 Kokusai Denshin Denwa Co Ltd SEMICONDUCTOR LASER WITH DISTRIBUTED FEEDBACK WITH MONITOR.

Also Published As

Publication number Publication date
JPS6320396B2 (en) 1988-04-27

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