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JPS6320396B2 - - Google Patents
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JPS6320396B2 - - Google Patents

Info

Publication number
JPS6320396B2
JPS6320396B2 JP56174107A JP17410781A JPS6320396B2 JP S6320396 B2 JPS6320396 B2 JP S6320396B2 JP 56174107 A JP56174107 A JP 56174107A JP 17410781 A JP17410781 A JP 17410781A JP S6320396 B2 JPS6320396 B2 JP S6320396B2
Authority
JP
Japan
Prior art keywords
semiconductor laser
region
laser device
current injection
active region
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
Application number
JP56174107A
Other languages
Japanese (ja)
Other versions
JPS5875877A (en
Inventor
Hidenori Nomura
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
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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
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)

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つ
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つ
て発振閾値が変化し従つ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オトダイオー
ドと共に使用し光出力を一定に保つためのバイア
ス電流調整回路が付加されていた。フオトダイオ
ードを半導体レーザ素子をモノリシツクに集積化
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 are small in size, have high power efficiency, have a long lifespan, and are easy to maintain, which are unmatched by other lasers, so in recent years their use as light sources for optical fiber communications and optical information processing has been increasingly widespread. However, semiconductor lasers have the characteristic that their oscillation threshold changes with changes in ambient temperature, and therefore their optical output varies. 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 keep the optical output constant. A semiconductor laser device with a built-in monitor is also known, which monolithically integrates a photodiode with a semiconductor laser device to reduce the number of steps required to assemble the device and to downsize 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オ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つてレーザ
を構成し、レーザとは分離されたフオトダイオー
ドを作つていた。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
通化されたフオトダイオードの光吸収部はフオト
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 the conventional semiconductor laser device with a built-in monitor, a monitor photodiode is formed in a cascade with the laser in the direction of the optical output beam of the laser. For this reason, in the prior art, the laser was constructed with an etched mirror surface whose characteristics were inferior to that of the cleavage plane of the crystal, and a photodiode was constructed separate from the laser. A mirror surface with poor characteristics causes deterioration of laser operation, and a photodiode's light absorption section, which is shared with the active layer of the laser operating section, has the drawback 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、半導体ヘテロ接合を含む半導
体多層構造を有して構成される電流注入形半導体
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
ス領域を含むフオ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 semiconductor laser device having a semiconductor multilayer structure including a semiconductor heterojunction, a base region formed of a collector electrode and a light absorption layer separated from a current injection electrode is provided. A semiconductor laser device with a built-in monitor is obtained, which is characterized in that a phototransistor structure including the above is integrated.

次に図面を参照して本発明を詳細に説明する。
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10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
体から成るクラツド領域12とそのクラツド領域
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によつて構成さ
れている。光吸収層13は結晶成長時にはクラツ
ド領域12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
及びクラツド領域12へつながる電流注入ストラ
イプ領域15をその内部に含んでいる。なお電流
注入用電極17とコレクタ電極18とは絶縁膜1
6によつ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(100)のInP単結晶で厚さ約70μm、活性領域
11は<011>方向に延びたストライプ状で幅2μ
m、厚さ0.15μm、発振波長1.3μmに相当する
In0.74Ga0.26As0.56P0.44、クラツド領域12は活性
領域11上の厚さが約2μmのZnドープInP、光吸
収層13は厚さ約1.5μm、吸収端波長1.35μmに
相当するIn0.72Ga0.28As0.62P0.38、電流注入ストラ
イプ領域15は深さ約2μmのZn拡散によつてp
形に反転されており、活性領域11を中心とする
幅約5μm、コレクタ領域14は深さ1μmのZn拡
散によつてp形に反転され電流注入ストライプ領
域15とは約10μmの間隔をおいて設けられた幅
約20μmのストライプ状、絶縁膜16は厚さ0.2μ
mのSiO2、電流注入用電極17とコレクタ電極
18は厚さ約0.3μmのAu−Zn合金、n側電極1
9は厚さ約0.3μmのAu−Sn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にへ
き開によつて切り出され、その共振器長は約
250μmである。
Next, the present invention will be explained in detail with reference to the drawings.
The drawing is a cross-sectional view perpendicular to the laser light output beam direction of one embodiment of the present invention. This embodiment includes an active region 11 formed on an n-type semiconductor substrate 10 and having a buried structure, a cladding region 12 made of a p-type semiconductor, a light absorption layer 13 on the cladding region 12, and an n-side electrode 19. It is composed of a current injection electrode 17 and a collector electrode 18. During crystal growth, the light absorption layer 13 is formed of an n-type conductivity type opposite to that of the cladding region 12, and then a collector region 14 is formed by thermal diffusion of p-type impurities.
and a current injection stripe region 15 connected to the cladding region 12. Note that the current injection electrode 17 and the collector electrode 18 are the insulating film 1.
6. To describe the composition and dimensions of each main part, the semiconductor substrate 10 is made of InP single crystal with a plane orientation of (100) and has a thickness of about 70 μm, and the active region 11 has a stripe shape extending in the <011> direction and has a width of 2 μm.
m, thickness 0.15μm, equivalent to oscillation wavelength 1.3μm
In 0.74 Ga 0.26 As 0.56 P 0.44 , the cladding region 12 is Zn-doped InP with a thickness of about 2 μm above the active region 11, and the light absorption layer 13 is In 0.72 Ga with a thickness of about 1.5 μm, corresponding to an absorption edge wavelength of 1.35 μm. 0.28 As 0.62 P 0.38 , the current injection stripe region 15 has a p
The collector region 14 has a width of about 5 μm centered on the active region 11 and is inverted to a p-type by Zn diffusion to a depth of 1 μm, and is spaced apart from the current injection stripe region 15 by about 10 μm. The insulating film 16 has a stripe shape with a width of about 20 μm and a thickness of 0.2 μm.
m SiO 2 , current injection electrode 17 and collector electrode 18 are Au-Zn alloy with a thickness of about 0.3 μm, n-side electrode 1
9 is an Au-Sn alloy with a thickness of about 0.3 μm. The device is cut out by cleavage in a direction perpendicular to the stripe direction of the active region 11, and its cavity length is approximately
It is 250 μm.

さて、電流注入用電極17に正電圧、n側電極
19に負電極を印加して、電流注入ストライプ領
域15及びクラツド領域12を通して活性領域1
1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1
8には負の電圧を印加しておく。活性領域11と
クラツド領域12の界面における光学的不完全性
によつて散乱されたレーザ光出力の一部はベース
領域13aで吸収され光励起電流を発生する。こ
の光励起電流はクラツド領域12及びベース領域
13a及びコレクタ領域14が構成するヘテロ接
合pnp形フオトトランジスタ構造の高い電流増幅
率によつて増幅されコレクタ電極18から取り出
される。フオトダイオードを集積化した従来例で
は、フオ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つたために、受光効率
が低く、小さなモニタ電流しか得られなかつたの
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オトトランジス
タ構造の高い増幅率によつ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、結晶のへき開によつて共振
器を形成できるという利点もある。
Now, by applying a positive voltage to the current injection electrode 17 and a negative electrode to the n-side electrode 19, a current injection stripe region 15 and a cladding region 12 are applied to the active region 1.
When a current is injected into 1, laser oscillation starts at a point where a current of 30 to 40 mA or more is injected. Collector electrode 1
8 is applied with a negative voltage. A portion of the laser light output scattered by optical imperfections at the interface between active region 11 and cladding region 12 is absorbed by base region 13a, generating a photoexcitation current. This photoexcitation current is amplified by the high current amplification factor of the heterojunction pnp type phototransistor structure constituted by the cladding region 12, the base region 13a, 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 receiving efficiency and only a small monitor current. In this embodiment, since the composition of the light absorption layer 13 can be optimized independently of the composition of the active region 11, high light receiving efficiency can be obtained, and furthermore, since the light is amplified by the high amplification factor of the phototransistor structure, slight scattering can be achieved. Sufficient monitor current can be obtained just by using light. 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ツド領域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素子の構造に関しても上述
の構造には限定されず、他の埋め込み構造でもよ
く、また活性層が平面的広がりを有する非埋め込
み構造でもよい。半導体材料は必ずしもInP/
InGaAsP系に限らずGaAs/GaAlAs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
良い。
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. Further, the structure of the current injection type semiconductor laser device is not limited to the above-mentioned structure, but may be any other buried structure, or may be a non-buried structure in which the active layer has a planar extent. Semiconductor materials are not necessarily InP/
The material is not limited to InGaAsP, but may be any material such as GaAs/GaAlAs that can form a semiconductor laser device.

最後に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、光出力の安定化に
とつ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 optical output can be obtained. It is something that can be done.

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

図面は一実施例の断面図である。 図中、10……半導体基板、11……活性領
域、12……クラツド領域、13……光吸収層、
13a……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。
The drawing is a cross-sectional view of one embodiment. In the figure, 10...semiconductor substrate, 11... active region, 12... cladding region, 13... light absorption layer,
13a...Base area, 14...Collector area,
15... Current injection stripe region, 16... Insulating film, 17... Current injection electrode, 18... Collector electrode, 19... N-side electrode.

Claims (1)

【特許請求の範囲】 1 半導体ヘテロ接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半導体レーザ素子にお
いて、該半導体レーザ素子の活性領域の上方に形
成されたクラツド層をエミツタ領域としかつ前記
活性領域を成す半導体に比べ小さな禁制帯幅と前
記クラツド層の反対導電形とを有して該クラツド
層上に形成された光吸収層中にベース領域及びコ
レクタ領域を有し該コレクタ領域が前記光吸収層
への不純物導入によつて電流注入部とは電気的に
分離された構造を有するフオ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。 2 前記電流注入形半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に設けられている
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. In a current injection type semiconductor laser device having a semiconductor multilayer structure including a semiconductor heterojunction, a cladding layer formed above an active region of the semiconductor laser device is used as an emitter region and A base region and a collector region are included in a light absorption layer formed on the cladding layer and have a smaller band gap than the semiconductor constituting the active region and a conductivity type opposite to that of the cladding layer. A semiconductor laser device with a built-in monitor, characterized in that a phototransistor structure having a structure electrically isolated from a current injection part by introducing an impurity into the light absorption layer is integrated. 2. The current injection type semiconductor laser device according to claim 1, wherein the current injection type semiconductor laser device has a buried structure active region, and the base region is provided at a position apart from above the active region. Semiconductor laser element with built-in monitor.
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 JPS5875877A (en) 1983-05-07
JPS6320396B2 true 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)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6079788A (en) * 1983-10-06 1985-05-07 Nec Corp Optical bistable element
JPH06105820B2 (en) * 1985-12-25 1994-12-21 国際電信電話株式会社 Distributed feedback type semiconductor laser with monitor

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1517537A (en) * 1975-07-16 1978-07-12 Post Office Lasers and photo-detectors

Also Published As

Publication number Publication date
JPS5875877A (en) 1983-05-07

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