JPS63262886A - Semiconductor laser device - Google Patents

Semiconductor laser device

Info

Publication number
JPS63262886A
JPS63262886A JP9900687A JP9900687A JPS63262886A JP S63262886 A JPS63262886 A JP S63262886A JP 9900687 A JP9900687 A JP 9900687A JP 9900687 A JP9900687 A JP 9900687A JP S63262886 A JPS63262886 A JP S63262886A
Authority
JP
Japan
Prior art keywords
side electrode
light
emitting region
active layer
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.)
Pending
Application number
JP9900687A
Other languages
Japanese (ja)
Inventor
Yousuke Yamamoto
山本 陽祐
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP9900687A priority Critical patent/JPS63262886A/en
Publication of JPS63262886A publication Critical patent/JPS63262886A/en
Pending legal-status Critical Current

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  • Semiconductor Lasers (AREA)

Abstract

PURPOSE:To reduce reactive currents, and to improve characteristics at the time of operation at high speed by forming one of p side or n side electrode for injecting carriers into a light-emitting region into the upper or lower region of the light-emitting region and near it. CONSTITUTION:An n side electrode 5a is shaped onto a main surface between two mesa grooves 6 in and near a region on a light-emitting region 1, and connected to a contact section 5b.When a p side electrode 3 is supplied with positive forward currents and the n side electrode 5a with negative ones, currents are constricted and flow through an active layer, and beams equal to the band gap of the active layer are generated in the light-emitting region 1, and projected as laser beams from an edge face. Since conductors are hardly shaped onto insulating films 4 on the outsides of the mesa grooves 6, however, capacitance between the electrodes 3, 4 is reduced, thus approximately diminishing reactive currents, which do not flow through the active layer, even when a device is operated at high speed, then stably working the device.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、高速動作を可能にした半導体レーザ装置に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a semiconductor laser device capable of high-speed operation.

〔従来の技術〕[Conventional technology]

第2図は、例えばJOtlRNAL OF LIGHT
W^VE TIC[1−NOLOGY、VOL、LT−
3,NO,5,0CTOBER19855AKAKIB
ARAet、 al 、:  InGaAsP P−S
UBS’l’RATE LASER3に示された従来の
半導体レーザ装置の構造を示す斜視図である。
Figure 2 shows, for example, JOtlRNAL OF LIGHT
W^VE TIC [1-NOLOGY, VOL, LT-
3,NO,5,0CTOBER19855AKAKIB
ARAet, al,: InGaAsP P-S
1 is a perspective view showing the structure of a conventional semiconductor laser device shown in UBS'l'RATE LASER3.

この図において、1は発光領域、2は半導体結晶層、3
はp6III電極、4は絶縁膜、5はn側電極、6はメ
サ溝で、共振器方向に沿って半導体結晶層2の発光領域
1の両側の部分に形成されている。
In this figure, 1 is a light emitting region, 2 is a semiconductor crystal layer, and 3 is a light emitting region.
4 is a p6III electrode, 4 is an insulating film, 5 is an n-side electrode, and 6 is a mesa groove, which are formed on both sides of the light emitting region 1 of the semiconductor crystal layer 2 along the cavity direction.

この構成では、p側電極3に正p r>@電極5に負の
順方向のバイアス電圧を印加すると、絶縁膜4によって
電流が狭窄され、活性H(図示せず)に電流が流れるこ
とにより発光領域1でそのエネルギーバンドギャップに
等しい光が生じ、端面よりレーザ光として出射される。
In this configuration, when a positive p r>@negative forward bias voltage is applied to the p-side electrode 3, the current is constricted by the insulating film 4, and the current flows through the active H (not shown). Light equal to the energy bandgap is generated in the light emitting region 1, and is emitted from the end face as a laser beam.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

上記のような従来の半導体レーザ装置は、メサ溝6の外
側のn側電極5とp611電極3との間に並列な容量が
存在するため、高速で動作させた場合、。
In the conventional semiconductor laser device as described above, since there is a parallel capacitance between the n-side electrode 5 outside the mesa groove 6 and the p611 electrode 3, when operated at high speed.

メサ溝6の外側のn側電極5とp側電極3の間を流れる
無効電流が増加し、高周波になるほど特性が悪化すると
いう問題点があった。
There is a problem in that the reactive current flowing between the n-side electrode 5 and the p-side electrode 3 outside the mesa groove 6 increases, and the characteristics deteriorate as the frequency increases.

この発明は、かかる問題点を解決するためになされたも
ので、活性層に流れない無効電流を低減して高速動作時
の特性を改善することができろ半導体レーザ装置を得る
乙とを目的とずろ。
This invention was made to solve this problem, and aims to provide a semiconductor laser device that can reduce the reactive current that does not flow through the active layer and improve the characteristics during high-speed operation. Zuro.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る半導体レーザ装置は、発光領域にキャリ
アを注入するためのp@電極またはn側電極の一方を、
発光領域上または発光領域下の領域およびその近傍にの
み形成したものである。
In the semiconductor laser device according to the present invention, one of the p@ electrode and the n-side electrode for injecting carriers into the light emitting region is
It is formed only in the region above or below the light emitting region and in the vicinity thereof.

〔作用〕[Effect]

この発明においては、p側電極とn側電極間の容量が小
さくなる。
In this invention, the capacitance between the p-side electrode and the n-side electrode is reduced.

[実施例] 第1図はこの発明の半導体レーザ装置の一実施例の構造
を示す斜視図である。
[Embodiment] FIG. 1 is a perspective view showing the structure of an embodiment of a semiconductor laser device of the present invention.

この図において、第2図と同一符号は同一部分を・示し
、5aはn#J電極で、発光領域1上の領域およびその
近傍の領域としての2本のメサ溝6の間の主面上に形成
されている。5bは前記発光領域1上の領域以外に形成
された配線のコンタクト部で、n#J電極5aと接続さ
れている。
In this figure, the same reference numerals as in FIG. is formed. Reference numeral 5b denotes a contact portion of a wiring formed in a region other than the region above the light emitting region 1, and is connected to the n#J electrode 5a.

この発明の半導体レーザ装置も従来のものと同様に、p
側電極3に正、n側電極5aに負の順方向のバイアス電
圧を印加すると、活性層(図示せず)に電光が狭窄され
て流れ、発光領域1でそのエネルギーバンドギャップに
等しい光が生じ、端面よりレーザ光として出射される・
The semiconductor laser device of this invention also has p
When a positive forward bias voltage is applied to the side electrode 3 and a negative forward bias voltage is applied to the n-side electrode 5a, electric light is constricted and flows through the active layer (not shown), and light equal to the energy band gap is generated in the light emitting region 1. , which is emitted from the end face as a laser beam.
.

しかし、この発明の半導体レーザ装置は、メサ溝6の外
側の絶縁膜4上に導体をほとんど形成していないので、
p側電極3とn側電極5a間の容量が従来の構造のもの
に較べて小さくなっている。
However, in the semiconductor laser device of the present invention, since almost no conductor is formed on the insulating film 4 outside the mesa groove 6,
The capacitance between the p-side electrode 3 and the n-side electrode 5a is smaller than that of the conventional structure.

このため、高速で動作させた場合でも、活性層に流れな
い無効電流がほとんど生じることがなくなり、安定に動
作する。
Therefore, even when operating at high speed, there is almost no generation of reactive current that does not flow through the active layer, and the device operates stably.

なお、上記実施例ではp型基板を用いて構成した半導体
レーザ装置について説明したが、この発明はn型基板を
用い、各半導体層の導電型を反対にして構成しても同様
の効果が得られろ。
In the above embodiment, a semiconductor laser device constructed using a p-type substrate was described, but the same effect can be obtained even if the present invention is constructed using an n-type substrate and the conductivity types of each semiconductor layer are reversed. Let it go.

また、上記実施例では活性層への電流がメサ溝6からそ
の外側に形成された絶縁膜4によって狭窄される構造の
半導体レーザ装置について述べたが、これ以外の構造、
例えばpn接合の逆バイアスにより電流が狭窄される構
造の半導体レーザ装置に適用してもよい。
Further, in the above embodiment, a semiconductor laser device having a structure in which the current to the active layer is constricted from the mesa groove 6 by the insulating film 4 formed on the outside thereof has been described; however, other structures may be used.
For example, the present invention may be applied to a semiconductor laser device having a structure in which current is constricted by reverse bias of a pn junction.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明したとおり、発光領域にキャリアを
注入するためのp側電極またはn側電極の一方を、発光
領域上または発光領域下の領域およびその近傍にのみ形
成したので、p側電極とn側電極間の容量が小さくなり
、高速動作時にも活性層に流れない無効電流が減少して
活性層に有効に電流が流れるようになり、安定に動作す
るという効果がある。
As explained above, in this invention, either the p-side electrode or the n-side electrode for injecting carriers into the light-emitting region is formed only on the light-emitting region or in the region below the light-emitting region and in the vicinity thereof. The capacitance between the n-side electrodes is reduced, and the reactive current that does not flow through the active layer is reduced even during high-speed operation, allowing current to flow effectively through the active layer, resulting in stable operation.

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

第1図は乙の発明の半導体レーデ装置の一実施例の構造
を示す斜視図、第2図は従来の半導体レーザ装置の構造
の一例を示す斜視図である。 図において、1は発光領域、2は半導体結晶層、3はp
#I電極、4は絶縁膜、5aはn側電極、5bは配線の
コンタクト部、6はメサ溝である。 なお、各図中の同一符号は同一または相当部分を示す。 代理人 大 岩 増 雄   (外2名)第2図 手続補正書(自発) 昭和  年  月  日 持許庁長宮殿 1、事件の表示   特願昭62−99008号2、発
明の名称   半導体レーザ装置3、補正をする者 事件との関係  特許出願人 住 所     東京都千代田区丸の内二丁目2番3号
名 称  (601)三菱電機株式会社代表者志岐守哉 4、代理人 住 所    東京都千代田区丸の内二丁目2番3号5
3、:)−゛3 5、補正の対象 明細書の発明の詳細な説明の欄1図面の簡単な説明の欄
および図面 6、補正の内容 (1)明細書第2頁3行、第5頁17行の「1は発光領
域」を、それぞれ「1は活性層(発光旬域)」と補正す
る。 (2)同じく第2頁9行、第4頁3〜4行の「ンi性層
(図示せず)」を、それぞれ「活性層1」と補正する。 (3)  同じく第2頁15〜16行のrp側電極3と
の間に並列な容量が」を、「p側電極3により活性層1
に並列に容量が」と補正する。 (4)  図面中、第1図を別紙のように補正する。 以上 第 1  図“ 4:詑妹腰
FIG. 1 is a perspective view showing the structure of an embodiment of the semiconductor laser device of the invention, and FIG. 2 is a perspective view showing an example of the structure of a conventional semiconductor laser device. In the figure, 1 is a light emitting region, 2 is a semiconductor crystal layer, and 3 is a p
#I electrode, 4 is an insulating film, 5a is an n-side electrode, 5b is a wiring contact portion, and 6 is a mesa groove. Note that the same reference numerals in each figure indicate the same or corresponding parts. Agent: Masuo Oiwa (2 others) Diagram 2 procedural amendment (voluntary) Showa year/month Date of the Office of the Director-General's Palace 1, Indication of case: Patent Application No. 1982-99008 2, Title of invention: Semiconductor laser device 3 , Relationship to the case of the person making the amendment Patent Applicant Address 2-2-3 Marunouchi, Chiyoda-ku, Tokyo Name (601) Mitsubishi Electric Corporation Representative Moriya Shiki 4, Agent Address Marunouchi, Chiyoda-ku, Tokyo 2-2-3-5
3, :)-゛3 5. Detailed Description of the Invention Column 1 of the Specification Subject to Amendment 1 Brief Description of the Drawing Column and Drawing 6 Contents of the Amendment (1) Page 2 of the Specification, Line 3, Line 5 "1 is the light-emitting region" on page 17 line is corrected to "1 is the active layer (light-emitting region)". (2) Similarly, "active layer (not shown)" in line 9 of page 2 and lines 3 to 4 of page 4 are corrected to "active layer 1". (3) Similarly, on page 2, lines 15 and 16, the term ``capacitance in parallel with the rp-side electrode 3'' was changed to ``the active layer 1 is connected to the p-side electrode 3''.
The capacitance is corrected in parallel to . (4) In the drawings, Figure 1 should be amended as shown in the attached sheet. Above is Figure 1 “4: Yoshikoshi

Claims (2)

【特許請求の範囲】[Claims] (1)発光領域にキャリアを注入するためのp側電極ま
たはn側電極の一方を、前記発光領域上または前記発光
領域下の領域およびその近傍にのみ形成したことを特徴
とする半導体レーザ装置。
(1) A semiconductor laser device characterized in that one of a p-side electrode and an n-side electrode for injecting carriers into a light-emitting region is formed only on the light-emitting region or in a region below the light-emitting region and in the vicinity thereof.
(2)電極が発光領域上または発光領域下の領域以外に
形成された配線のコンタクト部と接続されたものである
ことを特徴とする特許請求の範囲第(1)項記載の半導
体レーザ装置。
(2) The semiconductor laser device according to claim (1), wherein the electrode is connected to a contact portion of a wiring formed in a region other than above or below the light emitting region.
JP9900687A 1987-04-21 1987-04-21 Semiconductor laser device Pending JPS63262886A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9900687A JPS63262886A (en) 1987-04-21 1987-04-21 Semiconductor laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9900687A JPS63262886A (en) 1987-04-21 1987-04-21 Semiconductor laser device

Publications (1)

Publication Number Publication Date
JPS63262886A true JPS63262886A (en) 1988-10-31

Family

ID=14234950

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9900687A Pending JPS63262886A (en) 1987-04-21 1987-04-21 Semiconductor laser device

Country Status (1)

Country Link
JP (1) JPS63262886A (en)

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