JPH0414276A - Surface-emitting semiconductor laser element - Google Patents

Surface-emitting semiconductor laser element

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Publication number
JPH0414276A
JPH0414276A JP11719490A JP11719490A JPH0414276A JP H0414276 A JPH0414276 A JP H0414276A JP 11719490 A JP11719490 A JP 11719490A JP 11719490 A JP11719490 A JP 11719490A JP H0414276 A JPH0414276 A JP H0414276A
Authority
JP
Japan
Prior art keywords
film
layer
semiconductor laser
current
active layer
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
JP11719490A
Other languages
Japanese (ja)
Inventor
Shoji Kitamura
祥司 北村
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP11719490A priority Critical patent/JPH0414276A/en
Publication of JPH0414276A publication Critical patent/JPH0414276A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To reduce the diameter of the active area and threshold current of the title laser element by forming a high-resistance area in a part where the current of an active layer is narrowed by irradiating the part with protons. CONSTITUTION:The first reflecting mirror 2 of a multilayered film composed of 25 pairs of n-Al0.1Ga0.9As and AlAs layers formed by alternately piling up the layers, the first n-Al0.4Ga0.6As clad layer 3, and p-Al0.15Ga0.85As active layer 4 are successively formed on an n-GaAs semiconductor substrate 1. After the entire surface of this wafer is coated with an SiO2 film 3, the SiO2 film is removed by etching except the central part where the film 13 is left in a circular form. A high-resistance area 12 is formed in a part of the active layer 4 by irradiating the surface of the part with protons by using the SiO2 film 13 as a mask. In order to suppress the diffusion of the electric current at the p-n junction, the area 12 is formed to the top of the first clad layer 2. After the entire surface is again coated with another SiO2 film, the film is removed only from a circular part above a current constricting section and an AuZn/Au light emitting window is formed by using the remaining SiO2 film as a mask. Finally, the SiO2 mask is removed.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は半導体レーザ素子、特に面発光半導体レーザ素
子に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a semiconductor laser device, particularly a surface emitting semiconductor laser device.

〔従来の技術〕[Conventional technology]

面発光半導体レーザ素子は、基板表面に垂直な方向にレ
ーザ光を出射し、通常の半導体レーザ素子に比べて単一
継モード動作、大放射面積、狭出射角、および二次元ア
レー化が可能であるなど、多くの利点を有セすることか
ら近年開発が進められているものである。
Surface-emitting semiconductor laser devices emit laser light in a direction perpendicular to the substrate surface, and compared to normal semiconductor laser devices, they are capable of single-joint mode operation, large emission area, narrow emission angle, and two-dimensional array formation. It has been developed in recent years because it has many advantages such as:

この素子は基板に垂直に共振器を形成し、積層された半
導体膜の厚さ方向に光を共振させて、面方向にレーザ光
を出射する構造を持ち、電流狭窄機構の導入および半導
体多層膜反射鏡の高反射率化などにより低しきい値を得
ることができる。
This element has a structure in which a resonator is formed perpendicular to the substrate, and the light is resonated in the thickness direction of the stacked semiconductor films, and the laser light is emitted in the plane direction. A low threshold value can be obtained by increasing the reflectance of the reflecting mirror.

素子の作製は従来液相成長法が用いられてきたが、平坦
性、膜厚制御性および量産性に優れた有機金属気相成長
法(MOCVD法)を用いることにより、組成の異なる
半導体膜を交互に組み合わせた半導体多層膜反射鏡の形
成が容易であり、レーザ共振器を結晶中に内在させた構
造とすることが可能である。
Conventionally, liquid phase epitaxy has been used to fabricate devices, but by using metal organic chemical vapor deposition (MOCVD), which has excellent flatness, film thickness controllability, and mass production, it is now possible to fabricate semiconductor films with different compositions. It is easy to form semiconductor multilayer mirrors that are alternately combined, and it is possible to have a structure in which the laser resonator is embedded in the crystal.

第5図はMOCVD法を用いて作製した面発光半導体レ
ーザ素子の構成の一例を示した模式断面図である。第5
図において、二の半導体レーザ素子は、基板l上に化合
物半導体膜を積層形成したッドj13側に第1の半導体
多層膜反射鏡2、第2クラッド層5側に第2の半導体多
層膜反射鏡7を形成してあり、第2クラッド層5内に電
流狭窄層6を備えている。さらに第2の半導体多層膜反
射鏡7の上に光透過膜8とリング状のキャップ層9およ
びリング状の電極10を形成する。11は下側の電極で
ある。このような構造でレーザ光は中央部から素子の厚
さ方向と垂直な方向に出射される。
FIG. 5 is a schematic cross-sectional view showing an example of the structure of a surface-emitting semiconductor laser device manufactured using the MOCVD method. Fifth
In the figure, the second semiconductor laser element has a first semiconductor multilayer film reflection mirror 2 on the side of the pad j13 in which compound semiconductor films are laminated on the substrate l, and a second semiconductor multilayer film reflection mirror on the second cladding layer 5 side. A mirror 7 is formed, and a current confinement layer 6 is provided within the second cladding layer 5. Furthermore, a light transmitting film 8, a ring-shaped cap layer 9, and a ring-shaped electrode 10 are formed on the second semiconductor multilayer film reflecting mirror 7. 11 is a lower electrode. With such a structure, laser light is emitted from the center in a direction perpendicular to the thickness direction of the element.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

第5図のような面発光半導体レーザ素子を低しきい値と
するためには、活性領域の面積の拡がりを低減すること
が必要である。活性領域が円形の場合、例えば共振器長
L−7μ7活性層4の厚さd=3n、半導体多層膜反射
鏡2.7の反射*R= 0.95.温度300Kにおけ
るしきい値電流と活性領域の径の大きさは、第6図に示
す線図のような関係となる0面発光半導体レーザ素子で
は基板1に垂直方向に共振器を形成するため、活性層4
の厚A〜5−程度であり、第2クラッド層5内で電流狭
窄を行なう第5図のような構造では活性領域の径を低減
するのは容易でない。また、活性層4の中心部以外の領
域を高抵抗層やpn逆接合層で埋め込む構造を採用する
のは、活性層4の厚さからみても素子の製造工程が複雑
となり、歩留まりを低下させることになる。
In order to make the surface emitting semiconductor laser device as shown in FIG. 5 have a low threshold value, it is necessary to reduce the spread of the area of the active region. When the active region is circular, for example, the resonator length L-7μ7, the thickness d of the active layer 4 is 3n, and the reflection *R of the semiconductor multilayer film reflector 2.7 is 0.95. The relationship between the threshold current at a temperature of 300 K and the diameter of the active region is as shown in the diagram shown in FIG. active layer 4
In the structure shown in FIG. 5 in which current confinement is performed within the second cladding layer 5, it is not easy to reduce the diameter of the active region. Furthermore, adopting a structure in which regions other than the center of the active layer 4 are buried with a high-resistance layer or a pn reverse junction layer complicates the manufacturing process of the device, considering the thickness of the active layer 4, and reduces yield. It turns out.

本発明は上述の点に鑑みてなされたものであり、その目
的は埋め込み構造のような複雑な手段を用いることなく
、活性領域の径が小さく、しきい値電流の低い面発光半
導体レーザ素子を提供することにある。
The present invention has been made in view of the above points, and its purpose is to create a surface emitting semiconductor laser device with a small active region diameter and a low threshold current without using complicated means such as a buried structure. It is about providing.

〔課題を解決するための手段〕[Means to solve the problem]

上記の課題を解決するために本発明の面発光半導体レー
ザ素子は、活性層の電流を狭窄させる部分にプロトンを
照射して高抵抗領域を形成することにより、電流狭窄機
構を付与したものである。
In order to solve the above problems, the surface emitting semiconductor laser device of the present invention is provided with a current confinement mechanism by irradiating protons to the part of the active layer where the current is constricted to form a high resistance region. .

〔作用〕[Effect]

上記のように活性層の電流を狭窄させる部分に、プロト
ンを照射して高抵抗領域を形成した本発明の面発光半導
体レーザ素子は、埋め込み構造と同等の電流狭窄作用を
有し、素子の低しきい値電流を達成することができる。
The surface-emitting semiconductor laser device of the present invention, in which a high-resistance region is formed by irradiating protons to the current-confining portion of the active layer as described above, has a current confining effect equivalent to that of a buried structure, and reduces the A threshold current can be achieved.

〔実施例] 以下、本発明を実施例に基づき説明する。〔Example] Hereinafter, the present invention will be explained based on examples.

第1図は本発明の面発光半導体レーザ素子の構成を示す
模式断面図であり、第5図と共通部分を同一符号で表わ
して゛ある。第1図が第5図と異なる所は、活性層4に
プロトンを照射した高抵抗領域12を形成したことにあ
る。なお、電流狭窄層6を設けた構造は第4図に例示す
る。
FIG. 1 is a schematic cross-sectional view showing the structure of a surface-emitting semiconductor laser device of the present invention, and parts common to those in FIG. 5 are designated by the same reference numerals. The difference between FIG. 1 and FIG. 5 is that a high resistance region 12 is formed in the active layer 4 by irradiating protons. Incidentally, a structure in which the current confinement layer 6 is provided is illustrated in FIG.

次に第1図に示した本発明の面発光半導体レーザ素子の
製造方法について述べる。第2図(a)〜(C)はこの
素子をG5As / Aj G5As系の材料で構成し
たときの主な製造工程を示す模式断面図である。
Next, a method for manufacturing the surface emitting semiconductor laser device of the present invention shown in FIG. 1 will be described. FIGS. 2(a) to 2(C) are schematic cross-sectional views showing the main manufacturing steps when this element is constructed from a G5As/Aj G5As-based material.

まず、n−G5As半導体基板l (厚さ loom、
キャリア密度I X 1010l8a’)上にn −A
I 。、 +Ga、、wAsと〜Asを交互に25対積
層(各層厚はλ/4)した第1の多層膜反射@ 2 、
  n  N o、 4Ga6,6As (厚さIg、
キャリア密度I X 10+s cffl−″)の第1
 ’)ランド層3およびp  Al a、 +5Gao
、 gsAs (厚さ3−、キャリア密度I X 10
I?C1l −’ )の活性層4を順次形成する〔第2
図(a)〕。次にこのウェハ表面の全面をSiO□膜1
3で被覆した後、その中心部に10nΦの円形部分を残
し、その他の領域をエツチング除去する。そして1on
ΦのSing膜13をマスクとしてウェハ表面にプロト
ンを照射し、活性層4の一部に高抵抗領域12を形成す
る。このときpn接合における電流の拡がりを抑えるた
め、第1クラッド層3の上部まで高抵抗領域12となる
ようにする〔第2図Φ)〕。
First, the n-G5As semiconductor substrate l (thickness loom,
carrier density I x 1010l8a') on n - A
I. , +Ga,, 25 pairs of wAs and ~As are alternately laminated (each layer thickness is λ/4). First multilayer film reflection @ 2 ,
n No, 4Ga6,6As (thickness Ig,
carrier density I x 10+s cffl-'')
') Land layer 3 and p Al a, +5Gao
, gsAs (thickness 3−, carrier density I × 10
I? C1l-') active layer 4 is sequentially formed [second
Figure (a)]. Next, the entire surface of this wafer is covered with a SiO□ film 1.
After coating with No. 3, a circular portion of 10 nΦ is left in the center, and the other areas are etched away. And 1on
Using the Sing film 13 of Φ as a mask, the wafer surface is irradiated with protons to form a high resistance region 12 in a part of the active layer 4. At this time, in order to suppress the spread of current in the pn junction, the high resistance region 12 extends to the top of the first cladding layer 3 [FIG. 2 Φ].

次にSiO□膜13をエツチング除去後、P  JVo
、4Gao、hAs(厚さ1−、キャリア密度I X 
10111cs−3)の第2クラッド層5 、  p 
−Ai @、 lG30.9ASとA1Asを交互に2
5対積層(各層圧はλ/4)した第2の多層膜反射鏡7
 +  P  +’V++、 zG3o、o−s(厚さ
0.3nキャリア密度lXl0”ロー3)の光透過膜8
.p−GaAs (厚さ0.5ts、キャリア密度I 
X 1019cs−3)のキャップ層9を順次積層し、
さらにAuZn/Auの電極10を表面全面に形成する
〔第2図(C1)。
Next, after removing the SiO□ film 13 by etching, P JVo
, 4Gao, hAs (thickness 1-, carrier density I
10111cs-3) second cladding layer 5, p
-Ai @, lG30.9AS and A1As alternately 2
A second multilayer film reflecting mirror 7 with 5 pairs laminated (each layer pressure is λ/4)
+ P +'V++, zG3o, o-s (thickness 0.3n carrier density lXl0'' low 3) light transmitting film 8
.. p-GaAs (thickness 0.5ts, carrier density I
X 1019cs-3) cap layers 9 are sequentially laminated,
Furthermore, an electrode 10 of AuZn/Au is formed on the entire surface [FIG. 2 (C1)].

その後はSiO□膜を全面に付着した後、これを電流狭
窄部の上部のみフォトエツチングにより円形に除去し、
残りのSiO□膜をマスクとしてAuZn/Au電極1
0とp−GaAsキャップ層9までを除去して光出射窓
を形成し、最後にSiO□マスクを除去する。
After that, after depositing a SiO
AuZn/Au electrode 1 using the remaining SiO□ film as a mask
0 and p-GaAs cap layer 9 are removed to form a light exit window, and finally the SiO□ mask is removed.

その後、基板1側にAuGe/Au電極11を形成し、
ox/N8混合ガス雰囲気中で450°C110分間の
熱処理を施すことにより、第1図の構成を持つ面発光半
導体レーザ素子を得ることができる。
After that, an AuGe/Au electrode 11 is formed on the substrate 1 side,
By performing heat treatment for 110 minutes at 450° C. in an ox/N8 mixed gas atmosphere, a surface emitting semiconductor laser device having the structure shown in FIG. 1 can be obtained.

以上のようにして作製した本発明の面発光半導体レーザ
素子の室温における電流−光出力特性線図を第3図に示
す、第3図からしきい値電流は10−A程度となり、活
性層の一部にプロトンを照射し高抵抗領域を形成するこ
とにより、電流狭窄が有効に行われていることがわかる
FIG. 3 shows a current-light output characteristic diagram at room temperature of the surface-emitting semiconductor laser device of the present invention fabricated as described above. From FIG. 3, the threshold current is about 10-A, and the It can be seen that current confinement is effectively achieved by irradiating a portion with protons to form a high resistance region.

なお、第1図の素子構成において、基板lと半導体多層
膜反射#!2との間に厚さ0.5n、キャリア密度lX
l0”ロー3のn−GaAsバッファ層を設けてもよく
、また、活性層4の一部にプロトン照射を行なった後電
流狭窄層6を埋め込み、第4図のように第5図と同様の
構成とすることもでき、この場合電流狭窄層6による効
果も合わせて電流狭窄が確実に行われる。
In addition, in the device configuration shown in FIG. 1, the substrate l and the semiconductor multilayer film reflection #! 2, thickness 0.5n, carrier density lX
An n-GaAs buffer layer of 10" row 3 may be provided, and after proton irradiation is performed on a part of the active layer 4, a current confinement layer 6 is buried, as shown in FIG. 4 and similar to that in FIG. In this case, the current confinement is reliably performed together with the effect of the current confinement layer 6.

以上、GaAs / JV GaAs系の材料について
説明してきたが、その他の材料系を選択することができ
るのは勿論である。
Although GaAs/JV GaAs-based materials have been described above, it is of course possible to select other material systems.

〔発明の効果〕〔Effect of the invention〕

基板面と垂直な方向に共振器を持つ面発光半導体レーザ
素子は、そのしきい値電流を低くするための電流狭窄構
造とするのに、活性領域の径を小さくするとか、高抵抗
層を埋め込むなどの手段は、従来簡単に行なうことがで
きなかったが、本発明では活性層の一部をプロトン照射
して高抵抗開城を形成したために、埋め込み構造と同等
の十分な電流狭窄が可能となり、低しきい値電流の面発
光半導体レーザ素子を簡単なプロセスにより実現するこ
とができる。
Surface-emitting semiconductor laser devices that have a resonator in a direction perpendicular to the substrate surface have a current confinement structure to lower the threshold current by reducing the diameter of the active region or by embedding a high-resistance layer. Conventionally, such means could not be easily carried out, but in the present invention, a part of the active layer is irradiated with protons to form a high resistance open castle, so it is possible to achieve sufficient current confinement equivalent to that of a buried structure. A surface-emitting semiconductor laser device with a low threshold current can be realized by a simple process.

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

第1図は本発明の面発光半導体レーザ素子の構成を示す
模式断面図、第2図(a)〜(C)は本発明の面発光半
導体レーザ素子の主な製造工程を示す模式断面図、第3
図は本発明の面発光半導体レーザ素子の室温における電
流−光出力特性線図、第4図は電流狭窄層を付加した本
発明の面発光半導体レーザ素子の構成を示す模式断面図
、第5図は従来の面発光半導体レーザ素子の構成を示す
模式断面図、第6図は面発光半導体レーザ素子のしきい
値電流と活性領域の径の大きさとの関係を示す線図であ
る。 1:基板、2:第1の半導体多層膜反射鏡、3:第1ク
ラッド層、4:活性層、5:第2クラッド層、6:電流
狭窄層、7:第2の半導体多層膜反射鏡、8:光透過膜
、9:キャップ層、10.11  :第1図 第3図 第2図 第4図
FIG. 1 is a schematic cross-sectional view showing the structure of the surface-emitting semiconductor laser device of the present invention, and FIGS. 2(a) to (C) are schematic cross-sectional views showing the main manufacturing steps of the surface-emitting semiconductor laser device of the present invention. Third
The figure is a current-optical output characteristic diagram at room temperature of the surface-emitting semiconductor laser device of the present invention, FIG. 4 is a schematic cross-sectional view showing the structure of the surface-emitting semiconductor laser device of the present invention with a current confinement layer added, and FIG. 6 is a schematic cross-sectional view showing the structure of a conventional surface-emitting semiconductor laser device, and FIG. 6 is a diagram showing the relationship between the threshold current and the diameter of the active region of the surface-emitting semiconductor laser device. 1: Substrate, 2: First semiconductor multilayer film reflector, 3: First cladding layer, 4: Active layer, 5: Second cladding layer, 6: Current confinement layer, 7: Second semiconductor multilayer film reflector , 8: Light transmission film, 9: Cap layer, 10.11: Figure 1, Figure 3, Figure 2, Figure 4

Claims (1)

【特許請求の範囲】 1)半導体基板上に第1の半導体多層膜反射鏡、第1ク
ラッド層、活性層、第2クラッド層、第2の半導体多層
膜反射鏡を備えた面発光半導体レーザ素子であって、前
記活性層の電流を狭窄させる部分にプロトン照射により
形成された高抵抗領域を備えていることを特徴とする面
発光半導体レーザ素子。 2)半導体基板上に第1の半導体多層膜反射鏡、第1ク
ラッド層、活性層、第2クラッド層、第2の半導体多層
膜反射鏡を備え、前記第2クラッド層の一部に電流狭窄
層を有する面発光半導体レーザ素子であって、前記活性
層の電流を狭窄させる部分にプロトン照射により形成さ
れた高抵抗領域を備えていることを特徴とする面発光半
導体レーザ素子。
[Scope of Claims] 1) A surface-emitting semiconductor laser device comprising a first semiconductor multilayer reflector, a first cladding layer, an active layer, a second cladding layer, and a second semiconductor multilayer reflector on a semiconductor substrate. A surface-emitting semiconductor laser device, comprising a high-resistance region formed by proton irradiation in a portion of the active layer that constricts current. 2) A first semiconductor multilayer film reflector, a first cladding layer, an active layer, a second cladding layer, and a second semiconductor multilayer film reflector are provided on a semiconductor substrate, and current confinement is provided in a part of the second cladding layer. 1. A surface emitting semiconductor laser device having a layer, the surface emitting semiconductor laser device comprising a high resistance region formed by proton irradiation in a portion of the active layer that constricts current.
JP11719490A 1990-05-07 1990-05-07 Surface-emitting semiconductor laser element Pending JPH0414276A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11719490A JPH0414276A (en) 1990-05-07 1990-05-07 Surface-emitting semiconductor laser element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11719490A JPH0414276A (en) 1990-05-07 1990-05-07 Surface-emitting semiconductor laser element

Publications (1)

Publication Number Publication Date
JPH0414276A true JPH0414276A (en) 1992-01-20

Family

ID=14705728

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11719490A Pending JPH0414276A (en) 1990-05-07 1990-05-07 Surface-emitting semiconductor laser element

Country Status (1)

Country Link
JP (1) JPH0414276A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH09116227A (en) * 1995-10-20 1997-05-02 Nec Corp Surface emission type laser and its manufacture
JP2010126276A (en) * 2008-11-26 2010-06-10 Sakamoto Shokai:Kk Mobile crane

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH09116227A (en) * 1995-10-20 1997-05-02 Nec Corp Surface emission type laser and its manufacture
JP2010126276A (en) * 2008-11-26 2010-06-10 Sakamoto Shokai:Kk Mobile crane

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