JPH0328077B2 - - Google Patents

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Publication number
JPH0328077B2
JPH0328077B2 JP5327585A JP5327585A JPH0328077B2 JP H0328077 B2 JPH0328077 B2 JP H0328077B2 JP 5327585 A JP5327585 A JP 5327585A JP 5327585 A JP5327585 A JP 5327585A JP H0328077 B2 JPH0328077 B2 JP H0328077B2
Authority
JP
Japan
Prior art keywords
layer
semiconductor substrate
deposited
conductivity type
rectangular
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
JP5327585A
Other languages
Japanese (ja)
Other versions
JPS61214493A (en
Inventor
Kenichi Iga
Seiji Uchama
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.)
TOKYO KOGYO DAIGAKUCHO
Original Assignee
TOKYO KOGYO DAIGAKUCHO
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 TOKYO KOGYO DAIGAKUCHO filed Critical TOKYO KOGYO DAIGAKUCHO
Priority to JP5327585A priority Critical patent/JPS61214493A/en
Publication of JPS61214493A publication Critical patent/JPS61214493A/en
Publication of JPH0328077B2 publication Critical patent/JPH0328077B2/ja
Granted legal-status Critical Current

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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
    • H01S5/10Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
    • H01S5/18Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities
    • H01S5/183Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities having only vertical cavities, e.g. vertical cavity surface-emitting lasers [VCSEL]
    • H01S5/18305Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities having only vertical cavities, e.g. vertical cavity surface-emitting lasers [VCSEL] with emission through the substrate, i.e. bottom emission
    • 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
    • H01S2301/00Functional characteristics
    • H01S2301/16Semiconductor lasers with special structural design to influence the modes, e.g. specific multimode
    • H01S2301/163Single longitudinal mode
    • 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
    • H01S2301/00Functional characteristics
    • H01S2301/16Semiconductor lasers with special structural design to influence the modes, e.g. specific multimode
    • H01S2301/166Single transverse or lateral mode
    • 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
    • H01S5/0206Substrates, e.g. growth, shape, material, removal or bonding
    • H01S5/0207Substrates having a special shape
    • 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
    • H01S5/10Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
    • H01S5/18Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities
    • H01S5/183Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities having only vertical cavities, e.g. vertical cavity surface-emitting lasers [VCSEL]
    • 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
    • H01S5/2205Structure 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 comprising special burying or current confinement layers
    • H01S5/2214Structure 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 comprising special burying or current confinement layers based on oxides or nitrides
    • 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
    • H01S5/2205Structure 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 comprising special burying or current confinement layers
    • H01S5/2222Structure 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 comprising special burying or current confinement layers having special electric properties
    • H01S5/2224Structure 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 comprising special burying or current confinement layers having special electric properties semi-insulating semiconductors

Landscapes

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

Description

【発明の詳細な説明】 (技術分野) 本発明は、半導体基板上に形成したpnストラ
イプ構造による発振出力光を半導体基板に直角に
放射する面発光型レーザ素子およびその製造方法
に関し、特に、電流狭窄による発振電流閾値の低
減、横モード制御および縦単一モード化が可能な
高効率の面発光型レーザ素子を製造容易に構成し
たものである。
Detailed Description of the Invention (Technical Field) The present invention relates to a surface-emitting laser device that emits oscillation output light by a pn stripe structure formed on a semiconductor substrate at right angles to the semiconductor substrate, and a method for manufacturing the same, and in particular, This is a highly efficient surface-emitting laser element that can be easily manufactured and is capable of reducing the oscillation current threshold by confinement, controlling the transverse mode, and achieving a single longitudinal mode.

(従来技術) 従来のこの種面発光型レージ素子は、例えば、
第3図a〜dにそれぞれ示すように構成されてお
り、いずれも、その駆動電流乃至出力光のウエハ
面に対する横方向および縦方向の拡がりの姿勢、
すなわち、横モードおよび縦モードを制御してそ
れぞれ単一化するうえで難点があり、十分な性能
が得られない、という欠点があつた。
(Prior art) This kind of conventional surface-emitting type radiation device is, for example,
They are constructed as shown in FIGS. 3a to 3d, respectively, and in each case, the orientation of the horizontal and vertical spread of the drive current or output light with respect to the wafer surface,
That is, there is a drawback in that it is difficult to control and unify the transverse mode and the longitudinal mode, and sufficient performance cannot be obtained.

例えば、第3a図に示す構成の従来素子におい
ては、P側ミラー層110を兼ねるドツト状の金
属電流120を用いることのみによつて電流19
0の横方向の拡がりを制限しているので、活性領
域180において電流の著しい拡がりが生じ、電
流閾値の低減によるレーザに光の高効率化に限度
があり、また、P側ミラー層110の大きさを抑
えることのみによつては、出力光の横モード制御
も十分には行なえず、したがつて、電流狭窄構造
および光導波構造を別途設ける必要があつた。
For example, in the conventional element having the configuration shown in FIG. 3a, the current 19
Since the lateral spread of 0 is restricted, a significant spread of current occurs in the active region 180, which limits the ability to increase the efficiency of laser light by reducing the current threshold. The transverse mode control of the output light cannot be sufficiently controlled only by suppressing the light intensity, and therefore it is necessary to separately provide a current confinement structure and an optical waveguide structure.

その一例として、第3b図に示すような横接合
構造を有する従来素子が考えられた。すなわち、
例えば、同じn型のInPクラツド層30、
GaInAsP活性層40およびInP層50を積層して
かかる積層構造体の横方向の半分にZn拡散領域
200を設けてP形とし、同じ上面にミラー層1
10を挾んでP側電極層120とn側電極層14
0とを設けることにより、横方向の電流190を
制御し得るようにした面発光型レーザ素子が考え
られたが、かかる横接合構造では、上述したドツ
ト状ミラー構造におけると同様に、出力光の横モ
ードの制御性が不十分であつた。また、第3c図
に示すように、活性層40を中心にしたPn接合
積層構造体をクラツド層30の半ばまで蝕刻して
円形もしくは方形のメサ状にしたのち、その周囲
をpnpn多層InPストライプ埋込み層によつて囲ん
だ構成の従来素子においては、活性領域には電流
狭窄構造および出力光導波構造が存在在するが、
クラツド領域にはかかる狭窄構造および導波構造
が作用しないので、かかる多層埋込みによつて
も、矢張り、横モード制御性が不十分であつた。
さに、第3d図に示すように、上述したと同様の
円形もしくは方形のメサ構造の活性領域を囲む凹
欠部の内壁面に絶縁材被膜100を設けてメサ状
活性領域を絶縁膜100によつて囲んだ構成の従
来素子においては、電流狭窄および出力光導波の
構造は達成されるが、電流閾値を下げて高効率化
するためにメサの横断面積を小さくする必要があ
り、したがつて、小面積の金属材層をP側のミラ
ー110と電極120とに兼用せざるを得ず、P
側ミラー110を高反射率化することが困難とな
り、メサ構造の機械的強度が低下し、熱放散性が
劣化するなど、種々の問題が生じて、十分な性能
が得られなかつた。
As an example, a conventional element having a lateral junction structure as shown in FIG. 3b has been considered. That is,
For example, the same n-type InP cladding layer 30,
A GaInAsP active layer 40 and an InP layer 50 are laminated, and a Zn diffusion region 200 is provided in the lateral half of the laminated structure to form a P type, and a mirror layer 1 is formed on the same upper surface.
10, a P-side electrode layer 120 and an n-side electrode layer 14.
A surface-emitting laser device has been considered in which the lateral current 190 can be controlled by providing The controllability of the transverse mode was insufficient. In addition, as shown in FIG. 3c, the Pn junction stacked structure centered on the active layer 40 is etched to the middle of the cladding layer 30 to form a circular or rectangular mesa shape, and then the surrounding area is filled with pnpn multilayer InP stripes. In conventional devices with a structure surrounded by layers, a current confinement structure and an output optical waveguide structure exist in the active region.
Since the constriction structure and the waveguide structure do not act on the cladding region, even with such multilayer embedding, the transverse mode controllability was insufficient.
In addition, as shown in FIG. 3d, an insulating material film 100 is provided on the inner wall surface of the recess surrounding the active region of the circular or rectangular mesa structure similar to that described above, and the mesa-shaped active region is covered with the insulating film 100. In the conventional device with the enclosed structure, current confinement and output optical waveguide structure are achieved, but the cross-sectional area of the mesa needs to be reduced in order to lower the current threshold and improve efficiency. , it is necessary to use a metal material layer with a small area as both the mirror 110 and the electrode 120 on the P side.
Various problems such as difficulty in increasing the reflectance of the side mirror 110, a decrease in the mechanical strength of the mesa structure, and a deterioration in heat dissipation properties occurred, making it impossible to obtain sufficient performance.

(発明の目的) 本発明の目的は、上述した従来の欠点を除去す
るとともに従来の各種の電流狭窄構造の長所を巧
みに組合わせて、電流閾値の低減、横モード制御
および横モード単一化を併わせて可能にするとと
もに、良好な熱放散性および高い反射率をもつて
製造容易に構成した面発光型レーザ素子およびそ
の製造方法を提供することにある。
(Objective of the Invention) An object of the present invention is to eliminate the above-mentioned conventional drawbacks, and skillfully combine the advantages of various conventional current confinement structures to reduce the current threshold, control the transverse mode, and unify the transverse mode. It is an object of the present invention to provide a surface-emitting laser element that is easily manufactured and has good heat dissipation properties and high reflectance, and a method for manufacturing the same.

(発明の構成) すなわち、本発明面発光型レーザ素子は、いわ
ば、従来のストライプ構造による電流狭窄とメサ
構造による電流狭窄とを巧みに組合わせて電流お
よび光の双方を閉じ込め、電流閾値の低減のみな
らず、横モード制御および縦モード単一化を併わ
せて可能にしたものであり、円形もしくは方形の
開孔を有する半導体基板と、その半導体基板の前
記開孔を除く下面に被着した下側電極層と、前記
開孔に一致した同一形状の開口を設けて前記半導
体基板上に被着した当該半導体基板と同一導電型
の半導体材料よりなるエツチング停止層と、その
エツチング停止層上に前記開口を覆つて被着した
前記半導体基板と同一導電型の半導体材料よりな
るクラツド層と、そのクラツド層の下面に前記開
口を埋めて被着した下側ミラー層と、前記クラツ
ド層の一部を含むとともに前記半導体基板とは逆
導電型の半導体材料を備えた活性層を中心層とし
て前記開孔および前記開口に対向して位置する
pnストライプよりなる方形メサ構造と、そのメ
サ構造がなす方形の一方向に沿つた凹欠部を当該
方形メサ構造を挟んで設けるとともに少なくとも
当該方形メサ構造を覆う前記半導体基板とは逆導
電型の半導体材料層を最上層として前記クラツド
層上に被着したpn平面埋込み電流狭窄構造と、
そのpn平面埋込み電流狭窄構造上に被着した前
記半導体基板とは逆導電型の高濃度半導体材料よ
りなるキヤツプ層と、そのキヤツプ層上に前記方
形メサ構造に対向して被着した上側ミラー層と、
その上側ミラー層を囲んで前記キヤツプ層上に被
着した上側電極層とを備えたことを特徴とするも
のである。
(Structure of the Invention) In other words, the surface-emitting laser device of the present invention cleverly combines current confinement by the conventional stripe structure and current confinement by the mesa structure to confine both current and light, thereby reducing the current threshold. In addition, it is possible to control the transverse mode and unify the longitudinal mode. a lower electrode layer, an etching stop layer made of a semiconductor material of the same conductivity type as the semiconductor substrate and deposited on the semiconductor substrate with an opening having the same shape as the opening, and an etching stop layer formed on the etching stop layer. a cladding layer made of a semiconductor material of the same conductivity type as the semiconductor substrate deposited to cover the opening; a lower mirror layer deposited on the lower surface of the cladding layer filling the opening; and a part of the cladding layer. and an active layer including a semiconductor material having a conductivity type opposite to that of the semiconductor substrate is located as a central layer facing the opening and the opening.
A rectangular mesa structure consisting of a pn stripe, and a recess along one direction of the rectangle formed by the mesa structure are provided sandwiching the rectangular mesa structure, and the semiconductor substrate is of a conductivity type opposite to that of the semiconductor substrate that covers at least the rectangular mesa structure. a p-n plane buried current confinement structure deposited on the cladding layer with a semiconductor material layer as the top layer;
A cap layer made of a highly concentrated semiconductor material of a conductivity type opposite to that of the semiconductor substrate is deposited on the pn plane buried current confinement structure, and an upper mirror layer is deposited on the cap layer facing the square mesa structure. and,
It is characterized by comprising an upper electrode layer surrounding the upper mirror layer and deposited on the cap layer.

(実施例) 以下に図面を参照して実施例につき本発明を詳
細に説明する。
(Example) The present invention will be described in detail below with reference to the drawings.

しかして、本発明の特徴とするところの理解を
容易にするための説明の便宜上、最初に本発明面
発光型レーザ素子の製造過程の例を第1a図〜第
1h図に順次に示して詳述する。
Therefore, for the convenience of explanation to facilitate understanding of the features of the present invention, an example of the manufacturing process of the surface-emitting laser device of the present invention will first be shown in detail in FIGS. 1a to 1h. Describe.

すなわち、本発明レーザ素子の製造に当つて
は、まず、第1a図に示すように、例えば、n型
InP基板10上に、液相エピタキシヤル(LPE)
成長法、有機金属化学堆積(MOCVD)成長法、
分子線エピタキシヤル(MBE)成長法などの結
晶成長法により、後述の製造過程に必要なn型
GaInAsP材料よりなるエツチング停止層20に
引続いて、n型InP材料よりなるクラツド層3
0、p型GaInAsP材料よりなる活性層40およ
びP型InP層50を順次に成長させ、短共振器化
したpn接合層を積層堆積させる。ついで、かか
る堆積層を化学エツチンング法により、第1b図
に示すように、n型InPクラツド層30の半ばま
で蝕刻し、基板10上に適切なマトリツクス状に
点在した複数個の方形メサを形成する。ついで、
マトリツクス状に点在したそれら複数個の方形メ
サ群の相互間に、第1c図〜〜に示すよう
に、p型InP層60およびn型InP層70を交互
に積層して平面埋込みを施す。なお、第1c図
はpnp埋込み、珍図はpnpn多層埋込み、同図
はp埋込みの状態をそれぞれ示したものであり、
積層構造が複雑になるほどかかる埋込によるメサ
内電流狭窄作用の制御が容易となる。ついで、方
形メサ群に施したかかる平面埋込みにおける最上
層のp型InP層60上に、電極層との接触による
オーミツク抵抗を低減させるためのp型
GaInAsP材料よりなるキヤツプ層80を成長さ
せる。ついで、第1d図,に示すように、マ
トリツクス状に配列したメサ群間にマトリツクス
の一方向に沿つて化学エツチングを施し、各方形
メサの前後に埋込みストライプの部分を数μmず
つ残して凹欠部90を形成する。かかる凹欠部9
0の深さは、第1d図の線A−A′に沿つた同
図の断面図に示すようにn型InPクラツド層3
0の半ばまでとし、n型GaInAsPエツチング停
止層20には達しないようにする。第1d図に
示した凹欠部90の一部Bを拡大して同図に示
す。なお、図示の構造は、pnp埋込みを施した場
合の例を示したものである。ついで、第1e図に
示すように、各凹欠部90の内壁面に、例えば
SiO2やSi3N4などの材料からなる絶縁膜100を
被着して、凹欠部の蝕刻面に現われた半導体材
料、特にメサ内の半導体材料の露出面に化学的反
応が生じないようにするパツシベイシヨンを施
し、あるいは、ポリイミドなどの合成樹脂材料に
よつて各凹欠部90を平坦に埋込んでしまうよう
にする。
That is, in manufacturing the laser device of the present invention, first, as shown in FIG.
On the InP substrate 10, liquid phase epitaxial (LPE)
growth method, metal organic chemical deposition (MOCVD) growth method,
By crystal growth methods such as molecular beam epitaxial (MBE) growth, n-type
Following the etching stop layer 20 made of GaInAsP material, a cladding layer 3 made of n-type InP material
An active layer 40 and a P-type InP layer 50 made of a 0.0, p-type GaInAsP material are sequentially grown, and a pn junction layer having a short resonator is laminated. Next, the deposited layer is etched to the middle of the n-type InP cladding layer 30 by chemical etching, as shown in FIG. 1b, to form a plurality of rectangular mesas scattered in a suitable matrix on the substrate 10. do. Then,
Between the plurality of rectangular mesa groups scattered in a matrix, p-type InP layers 60 and n-type InP layers 70 are alternately stacked and buried in a plane, as shown in FIGS. In addition, Figure 1c shows the state of pnp embedding, the rare figure shows the state of pnpn multilayer embedding, and the same figure shows the state of p embedding.
The more complex the laminated structure is, the easier it becomes to control the current confinement in the mesa due to such embedding. Next, a p-type InP layer 60, which is the top layer of the planar embedding applied to the square mesa group, is coated with a p-type InP layer 60 to reduce ohmic resistance due to contact with the electrode layer.
A cap layer 80 of GaInAsP material is grown. Next, as shown in Fig. 1d, chemical etching is applied along one direction of the matrix between the mesa groups arranged in a matrix, leaving buried stripes of several micrometers at the front and back of each square mesa, and recesses are formed. A section 90 is formed. Such a recessed part 9
0 depth is the n-type InP cladding layer 3 as shown in the cross-sectional view of FIG. 1d along line A-A'.
0, so as not to reach the n-type GaInAsP etching stop layer 20. A part B of the recessed notch 90 shown in FIG. 1d is shown in an enlarged manner in the same figure. Note that the illustrated structure is an example in which PNP embedding is performed. Next, as shown in FIG. 1e, for example, the inner wall surface of each recessed notch 90 is
An insulating film 100 made of a material such as SiO 2 or Si 3 N 4 is deposited to prevent chemical reactions from occurring on the semiconductor material appearing on the etched surface of the recess, especially on the exposed surface of the semiconductor material in the mesa. The recessed portions 90 may be flattened or filled with a synthetic resin material such as polyimide.

以上のようにして形成した積層構造体において
個々にレーザ素子として作用すべき活性領域が存
在する方形メサの部分に対し、つぎのようにし
て、面発光型レーザ素子として作用するに必要な
構成要素を被着形成する。
In the laminated structure formed as described above, the components necessary for functioning as a surface-emitting laser element are added to the rectangular mesa portion in which the active region that individually functions as a laser element exists, as follows. Form the adhesion.

すなわち、第1f図に示すように、埋込みpn
ストライプと凹欠部とにより周囲を囲まれた方形
メサの部分におけるキヤツプ層80上に、誘電体
多層膜やAu薄膜などからなる高反射率のミラー
110を被着するとともに、埋込みpnストライ
プの部分におけるキヤツプ層80上には、AU/
Zn、Au/Cr、Ti/Pt/AUなどからなるp側電
極層120を被着する。一方、上述の積層構造体
の基板側背面には、第1g図に示すように、活性
領域が存在する方形メサの部分に対応して円形も
しくは方形の穴130を形成する。すなわち、該
当部分に選択エツチング法を適用して、まず、基
板10を構成するn型InP材料のみを腐蝕してエ
ツチング停止層20を構成するn型GaInAsP材
料は腐蝕しないエツチング液によつて基板10に
所要形状寸法の穴130を穿つた後に、エツチン
グ液を変えて穴底のエツチング停止層20を蝕刻
除去し、クラツド層30を露出させる。ついで、
基板10における穴130以外の部分の背面上に
AU/Sn、AU/Geなどからなるn側電型層14
0を被着するとともに、穴130の底面に露出し
たn型InPクラツド層30上には、積層構造体の
表面側に設けたミラー110と同様に誘電体多層
膜やAu薄膜などからなる高反射率のミラー15
0を被着する。
That is, as shown in Figure 1f, the embedded pn
A high-reflectance mirror 110 made of a dielectric multilayer film, an Au thin film, etc. is deposited on the cap layer 80 in the rectangular mesa area surrounded by the stripe and the recessed part, and the buried pn stripe area is coated on the cap layer 80. On the cap layer 80 of
A p-side electrode layer 120 made of Zn, Au/Cr, Ti/Pt/AU, etc. is deposited. On the other hand, as shown in FIG. 1g, a circular or square hole 130 is formed in the back side of the above-described laminated structure on the substrate side, corresponding to the part of the square mesa where the active region is present. That is, by applying a selective etching method to the relevant portion, first, the substrate 10 is etched using an etching solution that corrodes only the n-type InP material constituting the substrate 10 and does not corrode the n-type GaInAsP material constituting the etching stop layer 20. After drilling a hole 130 with a desired shape and size, the etching solution is changed to etch away the etching stop layer 20 at the bottom of the hole, exposing the cladding layer 30. Then,
On the back side of the part other than the hole 130 on the board 10
N-side type layer 14 made of AU/Sn, AU/Ge, etc.
At the same time, on the n-type InP cladding layer 30 exposed at the bottom of the hole 130, a highly reflective layer made of a dielectric multilayer film, a thin Au film, etc. is deposited, similar to the mirror 110 provided on the surface side of the laminated structure. rate mirror 15
Deposit 0.

以上のようにして多数のレーザ素子とマトリツ
クス配置した状態の積層構造体を第1h図,
に示すように、方形メサの部分を中心にした個々
のチツプに切り分けて、複数個の本発明面発光型
レーザ素子を一時に完成する。なお、第1h図
はレーザ素子チツプのP側を、同図はn側を、
いずれも上側にして示した概略斜視図であり、か
る製造過程により形成して横モード制御・電流狭
窄構造を有する本発明面発光型レーザ素子が得ら
れる。
Figure 1h shows the laminated structure in which a large number of laser elements and a matrix are arranged as described above.
As shown in FIG. 2, a plurality of surface-emitting laser devices of the present invention are completed at once by cutting into individual chips centered on the square mesa portion. Note that Fig. 1h shows the P side of the laser element chip, and the same figure shows the n side.
Both are schematic perspective views shown facing upward, and the surface-emitting laser device of the present invention having a transverse mode control/current confinement structure is obtained by forming the above manufacturing process.

上述のような製造過程により形成する本発明面
発光型レーザ素子の構成の例を改めて第2a図、
第2b図に示す。なお、第2a図は第1h図に
示したチツプの線A−A′に沿つた断面図であり、
また、第2b図は、同じチツプの線B−B′に沿
つた断面図である。図から明らかなように、本発
明面発光型レーザ素子において活性領域を擁する
方形メサの部分は、線A−A′の方向においては
pnストライプ埋込み層ににより、また、線B−
B′の方向においては化学エツチングにより形成
した凹欠部にパツシベイシヨンを施した絶縁材に
より、いずれも、電流および光の双方を閉じ込め
ており、したがつて、発振電流および発振出力光
の基板面に沿つた横方向の拡がりの姿勢を制御す
る横モード制御、並びに、基板面に垂直の方向の
拡がりの姿勢を制御する縦モード制御および単一
化の双方を、従来のように電流閾値低減の限度や
ミラー層の高反射率化の困難性あるいは熱放散性
の劣化やメサ構造の強度低下などの問題の発生を
伴うことなく、併わせて十分に達成することがで
きる。
An example of the configuration of the surface-emitting laser device of the present invention formed by the manufacturing process as described above is shown in FIGS. 2a and 2a.
It is shown in Figure 2b. Note that FIG. 2a is a cross-sectional view of the chip shown in FIG. 1h along line A-A',
FIG. 2b is a cross-sectional view of the same chip taken along line B--B'. As is clear from the figure, in the surface emitting laser device of the present invention, the part of the rectangular mesa containing the active region is in the direction of line A-A'.
Due to the pn stripe buried layer, the line B-
In the direction B', both current and light are confined by the insulating material applied to the recess formed by chemical etching, and therefore the oscillation current and the oscillation output light are transmitted to the substrate surface. Both lateral mode control, which controls the attitude of the spread in the horizontal direction along the substrate, and longitudinal mode control, which controls the attitude of the spread in the direction perpendicular to the substrate surface, and unification, are set to the current threshold reduction limit as in the past. This can be achieved satisfactorily without causing problems such as difficulty in increasing the reflectance of the mirror layer, deterioration of heat dissipation properties, and reduction in strength of the mesa structure.

かかる本発明面発光型レーザ素子の動作を第2
a図、第2b図に示した構成例について説明する
と、まず、p側およびn側の電極層120および
140の間に所定の直流電圧を印加して電流を流
すと、活性領域を擁する方形メサに流れる電流
は、pnストライプ埋込み層と凹込部90の内壁
面のパツシベイシヨン膜100とによつて囲まれ
た方形メサ内の活性領域に閉じ込められるので、
活性層40内にエネルギー準位に対する原子の分
布が反転したいわゆる反転分布が形成されて励起
されたレーザ光が発生する。その発生したレーザ
光も凹欠部90に囲まれて構成される導波路内に
閉じ込められ、その導波路の上下両端にそれぞれ
位置する高反射率のミラー110および150か
らなるフアブリペロー共振器によつて共振160
を起こし、レーザ発振が生ずる。その際、方形メ
サ内を流れる電流の閾値は、pnストライプ埋込
層60,70と凹欠部90のパツシベイシヨン膜
100とによる電流閉じ込め作用に基づいて十分
に低減される。また、出力レーザ光170は、活
性層40を中心として積層された短共振器により
縦単一モードを呈し、凹欠部90のパツシベイシ
ヨン膜100と方形メサがなす活性領域との材料
が呈する屈折率の差および活性領域の幅によつて
横単一モード化も可能となる。
The operation of the surface-emitting laser device of the present invention is described in a second manner.
To explain the configuration example shown in FIG. 2A and FIG. The current flowing through is confined in the active region within the rectangular mesa surrounded by the pn stripe buried layer and the passivation film 100 on the inner wall surface of the recess 90.
A so-called population inversion, in which the distribution of atoms with respect to energy levels is inverted, is formed in the active layer 40, and excited laser light is generated. The generated laser light is also confined within a waveguide surrounded by the concave cutout 90, and is confined by a Fabry-Perot resonator consisting of mirrors 110 and 150 with high reflectivity located at the upper and lower ends of the waveguide, respectively. resonance 160
This causes laser oscillation. At this time, the threshold value of the current flowing inside the rectangular mesa is sufficiently reduced based on the current confinement effect by the pn stripe buried layers 60 and 70 and the passivation film 100 of the recessed part 90. Further, the output laser beam 170 exhibits a single longitudinal mode due to the short resonators stacked around the active layer 40, and the refractive index exhibited by the material of the passivation film 100 of the concave cutout 90 and the active region formed by the rectangular mesa. A transverse single mode is also possible due to the difference in the width of the active region and the width of the active region.

また、第2図示の構成による本発明レーザ素子
は、凹欠部90およびその内壁面のパツシベイシ
ヨン膜100以外の部分を、第1図につき前述し
たように積層構造体にエツチングを施して方形メ
サを形成した後にpnストライプを埋込んで電流
狭窄構造を設ける製造過程の他、所要の堆積層を
適切に選択的に順次に被着することにより、積層
構造の半導体に作り付けの電流狭窄構造を設ける
ようにもなし得る構成上の利点を有している。
In addition, in the laser device of the present invention having the configuration shown in FIG. 2, a rectangular mesa is formed by etching the recessed portion 90 and the portions of its inner wall surface other than the passivation film 100 in the laminated structure as described above with reference to FIG. In addition to the manufacturing process that provides a current confinement structure by embedding pn stripes after formation, it is also possible to provide a built-in current confinement structure in a stacked semiconductor by appropriately selectively sequentially depositing the required deposited layers. It also has some structural advantages.

なお、以上の説明においては、n型InP基板か
ら出発した製造過程並びに素子構造の例について
述べたが、p形InP基板から出発し、以上の説明
における各層のp型とn型との設定をそれぞれ逆
にすることによつても、全く同様の製造過程によ
り全く同様の素子構造を有する本発明レーザ素子
を形成し得ること勿論である。また、各層の材料
についても、前述の例に限ることなく、例えば、
InPに替えてGaAsを用いるなど、適切な他の材
料を用いても同様に本発明レーザ素子を形成する
ことができる。
In addition, in the above explanation, we have described examples of the manufacturing process and element structure starting from an n-type InP substrate, but starting from a p-type InP substrate, the setting of p-type and n-type of each layer in the above explanation is also explained. Of course, by reversing each case, it is possible to form a laser device of the present invention having a completely similar device structure through a completely similar manufacturing process. In addition, the material of each layer is not limited to the above-mentioned example, for example,
The laser device of the present invention can be similarly formed using other suitable materials, such as using GaAs instead of InP.

(効果) 以上の説明から明らかなように、本発明によれ
ば、面発光型半導体レーザ素子において短共振器
化した活性領域に流れる電流にpnストライプ埋
込み層とパツシベイシヨンを施したエツチング溝
とにより十分に狭窄を施してその電流閾値を容易
に低減させ得るとともに、十分な横モード制御を
可能にして縦モードとともに横モードも単一化す
ることができ、したがつて、従来に比し格段に優
れた性能の面発光型レーザ素子を製造容易に実現
することができる。したがつて、光出力をウエハ
に対し十分に狭い拡がり角をもつて垂直に取出し
得る本発明の面発光型半導体レーザ素子によれ
ば、その2次元レーザ化や他の半導体機能素子と
の集積化も容易に実現することが可能となる。
(Effects) As is clear from the above description, according to the present invention, the pn stripe buried layer and the etched groove provided with passivation can effectively prevent the current flowing through the active region formed into a short cavity in a surface-emitting semiconductor laser device. It is possible to easily reduce the current threshold by narrowing the current, and also to enable sufficient transverse mode control to unify the transverse mode as well as the longitudinal mode. A surface-emitting laser device with improved performance can be easily manufactured. Therefore, according to the surface-emitting semiconductor laser device of the present invention, which can extract optical output perpendicularly to the wafer with a sufficiently narrow divergence angle, it is possible to convert it into a two-dimensional laser or integrate it with other semiconductor functional devices. can also be easily realized.

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

第1a図、第1b図、第1c図〜、第1d
図〜、第1e図〜第1g図および第1h図
,は本発明面発光レーザ素子の製造過程の例
を順次に示す断面図および斜視図、第2a図およ
び第2b図は本発明面発光型レーザ素子の構成例
を互いに直交する方向の断面についてそれぞれ示
す断面図、第3a図〜第3d図は従来の面発光型
レーザ素子の構成例をそれぞれ示す断面図であ
る。 10……n型InP基板、20……n型InPエツ
チング停止層、30……n型InPクラツド層、4
0……p型GaInAsP活性層、50……p型InP
層、60……p型InP埋込層、70……n型InP
埋込層、80……p型GaInAsPキヤツプ層、9
0……エツチング溝(凹欠部)、100……パツ
シベイシヨン膜、110……p側ミラー層、12
0……p側電極層、130……穴、140……n
側電極層、150……n側ミラー層、160……
光共振路、170……光出力、180……活性領
域、190……電流、200……Zn拡散領域。
Figure 1a, Figure 1b, Figure 1c~, Figure 1d
Figures 1e to 1g and 1h are sectional views and perspective views sequentially showing examples of the manufacturing process of the surface-emitting laser device of the present invention, and Figures 2a and 2b are surface-emitting laser devices of the present invention. FIGS. 3a to 3d are cross-sectional views showing examples of the structure of a conventional surface-emitting laser device, respectively, in cross-sections in directions perpendicular to each other. FIGS. 10... n-type InP substrate, 20... n-type InP etching stop layer, 30... n-type InP cladding layer, 4
0...p-type GaInAsP active layer, 50...p-type InP
layer, 60... p-type InP buried layer, 70... n-type InP
Buried layer, 80... p-type GaInAsP cap layer, 9
0... Etching groove (concave cutout), 100... Passivation film, 110... P-side mirror layer, 12
0...p-side electrode layer, 130...hole, 140...n
Side electrode layer, 150... n-side mirror layer, 160...
Optical resonance path, 170... optical output, 180... active region, 190... current, 200... Zn diffusion region.

Claims (1)

【特許請求の範囲】 1 円形もしくは方形の開孔を有する半導体基板
と、その半導体基板の前記開孔を除く下面に被着
した下側電極層と、前記開孔に一致した同一形状
の開口を設けて前記半導体基板上に被着した当該
半導体基板と同一導電型の半導体材料よりなるエ
ツチング停止層と、そのエツチング停止層上に前
記開口を覆つて被着した前記半導体基板と同一導
電型の半導体材料よりなるクラツド層と、そのク
ラツド層の下面に前記開口を埋めて被着した下側
ミラー層と、前記クラツド層の一部を含むととも
に前記半導体基板とは逆導電型の半導体材料を備
えた活性層を中心層として前記開孔および前記開
口に対向して位置するpnストライプよりなる方
形メサ構造と、そのメサ構造がなす方形の一方向
に沿つた凹欠部を当該方形メサ構造を挟んで設け
るとともに少なくとも当該方形メサ構造を覆う前
記半導体基板とは逆導電型の半導体材料層を最上
層として前記クラツド層上に被着したpn平面埋
込み電流狭窄構造と、そのpn平面埋込み電流狭
窄構造上に被着した前記半導体基板とは逆導電型
の高濃度半導体材料よりなるキヤツプ層と、その
キヤツプ層上に前記方形メサ構造に対向して被着
した上側ミラー層と、その上側ミラー層を囲んで
前記キヤツプ層上に被着した上側電極層とを備え
たことを特徴とする面発光型レーザ素子。 2 特許請求の範囲第1項記載のレーザ素子にお
いて、前記凹欠部の内壁面を絶縁材膜により被覆
したことを特徴とする面発光型レーザ素子。 3 特許請求の範囲第1項記載のレーザ素子にお
いて、前記凹欠部に合成樹脂材を充填したことを
特徴とする面発光型レーザ素子。 4 半導体基板上に、その半導体基板と同一導電
型の半導体材料よりなるエツチング停止層および
前記半導体基板と同一導電型の半導体材料よりな
るクラツド層を最下層とするとともに前記半導体
基板とは逆導電型の半導体材料を備えた活性層を
中心層としたpnストライプ構造を順次に成長さ
せて被着する成長過程と、前記pnストライプ構
造を前記クラツド層中まで化学エツチングにより
除去してマトリツクス状に配列した複数個のpn
ストライプ方形メサ構造を形成するメサ形成過程
と、少なくとも、前記複数個の方形メサ構造を覆
う前記半導体基板とは逆導電型の半導体材料層よ
りなるpn埋込み層により前記複数個の方形メサ
構造の間を平坦に埋込む平面埋込み過程と、その
平面埋込み層上に前記半導体基板とは逆導電型の
高濃度半導体材料よりなるキヤツプ層を成長させ
て被着するオーミツク抵抗低減過程と、前記平面
埋込み層および前記キヤツプ層を前記クラツド層
中まで化学エツチングにより除去して前記複数個
の方形メサ構造の相互間に前記マトリツクスの一
方向に沿つた凹欠部をそれぞれ形成するととも
に、それらの凹欠部の内壁面に絶縁材膜をそれぞ
れ被着し、もしくは、それらの凹欠部に合成樹脂
材をそれぞれ充填する電流狭窄過程と、前記複数
個の方形メサ構造にそれぞれ対向して前記キヤツ
プ層上に複数個の上側ミラー層を被着するととも
にそれら複数個の上側ミラー層をそれぞれ囲んで
前記キヤツプ層上に上側電極層を被着する上側共
振構造形成過程と、前記半導体基板および前記エ
ツチング停止層を選択エツチングにより下面から
順次に除去して前記複数個の方形メサ構造にそれ
ぞれ対向したそれぞれ複数個の開孔および開口を
円形もしくは方形に形成し、それらの開口にそれ
ぞれ露出した前記クラツド層の下面に複数個の下
側ミラー層を被着するとともに、それらの開孔を
除く前記半導体基板の下面に下側電極層を被着す
る下側共振構造形成過程と、前記半導体基板を前
記複数個の方形メサ構造をそれぞれ中心にして切
り分けるチツプ形成過程とを設けたことを特徴と
する面発光型レーザ素子の製造方法。
[Claims] 1. A semiconductor substrate having a circular or rectangular opening, a lower electrode layer deposited on the lower surface of the semiconductor substrate excluding the opening, and an opening having the same shape as the opening. an etching stop layer made of a semiconductor material of the same conductivity type as the semiconductor substrate and deposited on the semiconductor substrate; and a semiconductor of the same conductivity type as the semiconductor substrate deposited on the etching stop layer to cover the opening. a lower mirror layer deposited on the lower surface of the cladding layer to fill the opening, and a semiconductor material that includes a part of the cladding layer and has a conductivity type opposite to that of the semiconductor substrate. A rectangular mesa structure with the active layer as a central layer and consisting of the aperture and a pn stripe located opposite to the aperture, and a recess along one direction of the rectangle formed by the mesa structure with the rectangular mesa structure sandwiched therebetween. a pn plane buried current confinement structure deposited on the cladding layer with a semiconductor material layer of a conductivity type opposite to that of the semiconductor substrate as the uppermost layer covering at least the square mesa structure; a cap layer made of a highly concentrated semiconductor material of a conductivity type opposite to that of the deposited semiconductor substrate; an upper mirror layer deposited on the cap layer facing the square mesa structure; and a cap layer surrounding the upper mirror layer. A surface emitting laser device comprising: an upper electrode layer deposited on the cap layer. 2. A surface-emitting laser device according to claim 1, wherein the inner wall surface of the recessed portion is covered with an insulating material film. 3. A surface-emitting laser device according to claim 1, wherein the recessed portion is filled with a synthetic resin material. 4. On a semiconductor substrate, an etching stop layer made of a semiconductor material of the same conductivity type as the semiconductor substrate and a cladding layer made of a semiconductor material of the same conductivity type as the semiconductor substrate are provided as the bottom layer, and the etching stop layer is of a conductivity type opposite to that of the semiconductor substrate. A growth process in which a pn stripe structure is sequentially grown and deposited with an active layer having a semiconductor material as a central layer, and the pn stripe structure is removed by chemical etching into the cladding layer and arranged in a matrix. multiple pn
A mesa formation process for forming a striped rectangular mesa structure, and at least a pn buried layer made of a semiconductor material layer of a conductivity type opposite to that of the semiconductor substrate, which covers the plurality of rectangular mesa structures, between the plurality of rectangular mesa structures. a planar embedding process in which the planar embedding layer is buried flatly; an ohmic resistance reduction process in which a cap layer made of a highly concentrated semiconductor material of a conductivity type opposite to that of the semiconductor substrate is grown and deposited on the planar embedding layer; and removing the cap layer into the cladding layer by chemical etching to form recesses along one direction of the matrix between the plurality of rectangular mesa structures; A current confinement process in which an insulating material film is applied to each inner wall surface or a synthetic resin material is filled in each of the recesses, and a plurality of insulating material films are applied on the cap layer facing each of the plurality of rectangular mesa structures. an upper resonant structure formation process of depositing a plurality of upper mirror layers and depositing an upper electrode layer on the cap layer surrounding each of the plurality of upper mirror layers, and selecting the semiconductor substrate and the etching stop layer. A plurality of holes and openings are formed in a circular or rectangular shape each facing the plurality of rectangular mesa structures by sequentially removing them from the bottom surface by etching, and a plurality of holes and openings are formed in the bottom surface of the cladding layer exposed in each of the openings. a lower resonant structure forming step of depositing a lower mirror layer of the plurality of rectangular mesas and a lower electrode layer on the lower surface of the semiconductor substrate excluding the openings; 1. A method for manufacturing a surface-emitting laser device, comprising a step of forming chips in which the chips are cut into pieces centering on each structure.
JP5327585A 1985-03-19 1985-03-19 Surface light-emission type laser element and manufacture thereof Granted JPS61214493A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5327585A JPS61214493A (en) 1985-03-19 1985-03-19 Surface light-emission type laser element and manufacture thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5327585A JPS61214493A (en) 1985-03-19 1985-03-19 Surface light-emission type laser element and manufacture thereof

Publications (2)

Publication Number Publication Date
JPS61214493A JPS61214493A (en) 1986-09-24
JPH0328077B2 true JPH0328077B2 (en) 1991-04-17

Family

ID=12938184

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5327585A Granted JPS61214493A (en) 1985-03-19 1985-03-19 Surface light-emission type laser element and manufacture thereof

Country Status (1)

Country Link
JP (1) JPS61214493A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2717213B2 (en) * 1988-08-09 1998-02-18 科学技術振興事業団 Surface-emitting type semiconductor laser device
US4999843A (en) * 1990-01-09 1991-03-12 At&T Bell Laboratories Vertical semiconductor laser with lateral electrode contact
JPH0456182A (en) * 1990-06-21 1992-02-24 Hikari Gijutsu Kenkyu Kaihatsu Kk Manufacture of surface light-emitting semiconductor element

Also Published As

Publication number Publication date
JPS61214493A (en) 1986-09-24

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