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JPH10209561A - Semiconductor laser device - Google Patents

Semiconductor laser device

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Publication number
JPH10209561A
JPH10209561A JP1094897A JP1094897A JPH10209561A JP H10209561 A JPH10209561 A JP H10209561A JP 1094897 A JP1094897 A JP 1094897A JP 1094897 A JP1094897 A JP 1094897A JP H10209561 A JPH10209561 A JP H10209561A
Authority
JP
Japan
Prior art keywords
layer
semiconductor
carrier concentration
conductivity type
grown
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP1094897A
Other languages
Japanese (ja)
Other versions
JP3877823B2 (en
Inventor
Toru Haga
芳賀  徹
Toshihiro Kono
敏弘 河野
Satohiko Oka
聡彦 岡
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP01094897A priority Critical patent/JP3877823B2/en
Publication of JPH10209561A publication Critical patent/JPH10209561A/en
Application granted granted Critical
Publication of JP3877823B2 publication Critical patent/JP3877823B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Semiconductor Lasers (AREA)

Abstract

(57)【要約】 【課題】リーク電流を低減した低閾値埋込ヘテロレーザ
を提供する。 【解決手段】変曲点の無い滑らかな側面形状を持つメサ
ストライプを形成し、最初にp型InP層を埋め込み成
長し、次に成長するn型InP層(n−InP電流ブロ
ック層)を、第1及び、第1のキャリア濃度よりも大き
い第2のキャリア濃度の層からなり、この順序で成長す
る2層構造とし、その後、埋め込むp型InP層のキャ
リア濃度を第2のキャリア濃度以上とし、さらにn型I
nP層で埋め込む。
(57) Abstract: A low-threshold buried heterolaser with reduced leakage current is provided. A mesa stripe having a smooth side surface shape without an inflection point is formed, a p-type InP layer is first buried and grown, and then an n-type InP layer (n-InP current block layer) to be grown is formed. It has a two-layer structure consisting of a first and a second carrier concentration layer higher than the first carrier concentration and grown in this order, and then the carrier concentration of the p-type InP layer to be embedded is set to be equal to or higher than the second carrier concentration. , And n-type I
It is embedded with an nP layer.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は半導体レーザに関す
る。
[0001] The present invention relates to a semiconductor laser.

【0002】[0002]

【従来の技術】半導体レーザの低閾値化を達成するため
には、活性領域以外を流れるリーク電流の低減が必須で
ある。埋込ヘテロ(BH;Buried Heterostructure)構
造レーザでは、従来電流ブロック層としてp−n接合や
高抵抗半導体層(Fe及びTiドープ等)が用いられて
おり、p基板を用いたBHレーザの例は、エレクトロニ
クス・レターズ 28巻 ナンバー19 1992年
1844頁(ElectronicsLetters Vol.28 No.19 1992 p.
1844)に記載のように、有機金属気相成長(MOCV
D;Metalorganic Chemical Vapor Deposition)法によ
るp−n接合埋込型のBHレーザがある。
2. Description of the Related Art In order to lower the threshold value of a semiconductor laser, it is essential to reduce leakage current flowing in areas other than the active region. In a buried heterostructure (BH) laser, a pn junction or a high-resistance semiconductor layer (Fe and Ti doping) is conventionally used as a current blocking layer. An example of a BH laser using a p substrate is as follows. , Electronics Letters, Volume 28, Number 19, 1992
1844 (Electronics Letters Vol. 28 No. 19 1992 p.
1844), metal organic chemical vapor deposition (MOCV)
D: Metal organic Chemical Vapor Deposition) method, there is a pn junction buried BH laser.

【0003】[0003]

【発明が解決しようとする課題】従来技術でp−n接合
埋込によるBHレーザを作製すると、図2に示すように
n型InP埋込層6とn型InP層9,10がつながり
易く(n−n接続ができ易く)、電流がこのn−n接続
を通じて流れるため充分な低閾値化ができない。
When a BH laser with a pn junction is buried in the prior art, the n-type InP buried layer 6 and the n-type InP layers 9 and 10 are easily connected as shown in FIG. nn connection is easily formed), and a current cannot be reduced sufficiently because the current flows through the nn connection.

【0004】本発明の目的は、このようなn−n接続の
無い低リーク電流埋込構造を達成することにより、BH
レーザの低閾値化を図ることにある。
An object of the present invention is to achieve a low leakage current buried structure without such an nn connection, thereby achieving a BH
The object is to reduce the threshold of the laser.

【0005】[0005]

【課題を解決するための手段】上記目的を達成するため
の手段を、図1により説明する。変曲点の無い滑らかな
側面形状を持つメサストライプを形成し、その埋込成長
で最初にZnドープp型InP層5を、次にSiドープ
n型InP層6,7(n−InP電流ブロック層),Z
nドープp型InP層8,Siドープn型InP層9を
連続して成長する。これらの層のキャリア濃度の大きさ
は、n型InP層6<n型InP層7<p型InP層8
とする。
Means for achieving the above object will be described with reference to FIG. A mesa stripe having a smooth side surface shape without an inflection point is formed. In the buried growth, a Zn-doped p-type InP layer 5 is first formed, and then a Si-doped n-type InP layer 6, 7 (n-InP current block) is formed. Layer), Z
An n-doped p-type InP layer 8 and a Si-doped n-type InP layer 9 are continuously grown. The carrier concentration of these layers is such that n-type InP layer 6 <n-type InP layer 7 <p-type InP layer 8
And

【0006】この時、図1(a)に示すように、最初に
成長したp型InP層5によって結晶成長速度の遅い結
晶面が完全に形成されず、次に成長するn型InP層の
成長初期にその成長フロントがメサ最上部に達してしま
う場合がある。その場合でも、n型InP層6,7のキ
ャリア濃度がp型InP層8よりも小さいために、図1
(b)に示すように、p型InP層8からのZnの拡散
によりn型InP層6,7上部のキャリアが相殺され
て、メサ最上部に達した成長フロント部は有効な電流リ
ーク経路とはならない。
At this time, as shown in FIG. 1A, the crystal plane having a low crystal growth rate is not completely formed by the p-type InP layer 5 which has been grown first, and the growth of the n-type InP layer to be grown next. Initially, the growth front may reach the top of the mesa. Even in that case, since the carrier concentration of the n-type InP layers 6 and 7 is lower than that of the p-type InP layer 8, the structure shown in FIG.
As shown in (b), the carriers on the n-type InP layers 6 and 7 are offset by the diffusion of Zn from the p-type InP layer 8, and the growth front part reaching the top of the mesa becomes an effective current leakage path. Not be.

【0007】すると、n−InP電流ブロック層17
(Siドープn型InP層6,7からZnが拡散したI
nP層16を除いた部分)は、後にこの上方に成長する
n型InP層9又は10と分離された構造となる。
Then, the n-InP current blocking layer 17
(I where Zn is diffused from Si-doped n-type InP layers 6 and 7)
The portion excluding the nP layer 16) has a structure that is separated from the n-type InP layer 9 or 10 which grows above the portion later.

【0008】このような構造では、メサストライプの活
性領域以外を流れるリーク電流は効果的に抑止され、低
閾値半導体レーザが実現できる。
With such a structure, a leak current flowing in areas other than the active region of the mesa stripe is effectively suppressed, and a low threshold semiconductor laser can be realized.

【0009】[0009]

【発明の実施の形態】本発明をInGaAsP系BHレ
ーザに適用した場合について、図1,図3により説明す
る。
DESCRIPTION OF THE PREFERRED EMBODIMENTS A case where the present invention is applied to an InGaAsP-based BH laser will be described with reference to FIGS.

【0010】有機金属気相成長(MOCVD)法によ
り、p−InP基板1(キャリア濃度4〜6E18cm
~2)にp−InPクラッド層2(キャリア濃度〜1E1
8cm~2,厚さ〜2μm)を成長した後InGaAsP/InGaAs
MQW活性層3(波長1.3μm,厚さ〜0.2μm
)、n−InPクラッド層4(キャリア濃度〜2E1
8cm~2,厚さ〜1μm)を成長する。この時活性層3は
InGaAsP バルク活性層でも良く、MQW構造に限定され
ない。
A p-InP substrate 1 (carrier concentration of 4 to 6E18 cm) is formed by metal organic chemical vapor deposition (MOCVD).
~ 2 ) in the p-InP cladding layer 2 (carrier concentration ~ 1E1)
After growing 8cm ~ 2 , thickness ~ 2μm), InGaAsP / InGaAs
MQW active layer 3 (wavelength: 1.3 μm, thickness: 0.2 μm
), N-InP cladding layer 4 (carrier concentration 22E1)
8cm ~ 2 , thickness ~ 1μm). At this time, the active layer 3
An InGaAsP bulk active layer may be used and is not limited to the MQW structure.

【0011】その後、CVD法によりSiO2 膜15を
被着し、ホトリソグラフィー工程を経た後、SiO2
15をマスクとしてウェットエッチングにより図3に示
されるような変曲点の無い滑らかな側面を有するメサス
トライプを形成する。メサストライプはSiO2膜15
下部が側面からエッチングされ、SiO215膜がオー
バーハング状になるようにする。また活性層幅は1〜2
μm、メサ深さは2.5〜4μmである。
After that, a SiO 2 film 15 is deposited by the CVD method, and after a photolithography process, a smooth side surface having no inflection point as shown in FIG. 3 is formed by wet etching using the SiO 2 film 15 as a mask. A mesa stripe is formed. Mesa stripe is SiO 2 film 15
The lower portion is etched from the side so that the SiO 2 15 film becomes overhanging. The width of the active layer is 1-2.
μm and the mesa depth is 2.5-4 μm.

【0012】次にMOCVD法により、SiO2 膜15
を被着したままメサストライプの側面を、Znドープp
−InP層5(キャリア濃度〜1E18cm~2,厚さ0.
5 〜1μm),Siドープn−InP層6(キャリア
濃度〜1.5E18cm~2 ,厚さ0.2〜0.5μm),S
iドープn−InP層7(キャリア濃度〜2E18cm
~2,厚さ0.5 〜1μm)で埋め込む。
Next, the SiO 2 film 15 is formed by MOCVD.
While the side surface of the mesa stripe is
-InP layer 5 (carrier concentration ~1E18cm ~ 2, a thickness of 0.
5 to 1 μm), Si-doped n-InP layer 6 (carrier concentration: 1.5E18 cm 2 , thickness: 0.2 to 0.5 μm), S
i-doped n-InP layer 7 (carrier concentration 22E18 cm)
2 and a thickness of 0.5 to 1 μm).

【0013】その後Znドープp−InP層8(キャリ
ア濃度2E18cm~2以上,厚さ1〜3μm),Siドー
プn−InP層9(キャリア濃度〜2E18cm~2,厚さ
〜0.5μm )を成長し、メサストライプを埋め込ん
だ。n−InP層9はp−n接合と再成長界面を分離す
るために設けたもので、本発明では特に挿入を限定され
るものではない。
Thereafter, a Zn-doped p-InP layer 8 (carrier concentration of 2E18 cm to 2 or more, thickness of 1 to 3 μm) and a Si-doped n-InP layer 9 (carrier concentration of 2E18 cm to 2 and thickness of 0.5 μm) are grown. And embedded a mesa stripe. The n-InP layer 9 is provided for separating the pn junction and the regrowth interface, and the insertion is not particularly limited in the present invention.

【0014】次に、SiO2 膜を除去した後n−InP
層10(キャリア濃度〜2E18cm~2,厚さ〜2μ
m),n−InGaAsPキャップ層11(キャリア濃
度5E18cm~2以上,厚さ〜0.2μm )で平坦に埋め
込んだ。
Next, after removing the SiO 2 film, the n-InP
Layer 10 (carrier concentration ~ 2E18cm ~ 2 , thickness ~ 2μ)
m), n-InGaAsP cap layer 11 (carrier concentration 5E18 cm ~ 2 or more, they flatly embedded in thick ~0.2μm).

【0015】以上のようにして埋め込んだ構造では、図
1(a)に示すように、最初に成長したp型InP層5に
よって結晶成長速度の遅い結晶面が完全に形成されず、
次に成長するn型InP層の成長初期にその成長フロン
トがメサ最上部に達してしまう場合がある。その場合で
も、n型InP層6,7のキャリア濃度がp型InP層
8よりも小さいために、図1(b)に示すように、p型
InP層8からのZnの拡散によりn型InP層6,7
上部のキャリアが相殺されて、メサ最上部に達した成長
フロント部は有効な電流リーク経路とはならない。
In the structure buried as described above, as shown in FIG. 1A, a crystal plane having a low crystal growth rate is not completely formed by the p-type InP layer 5 grown first.
The growth front of the n-type InP layer to be grown next may reach the top of the mesa in the early stage of growth. Even in this case, since the carrier concentration of the n-type InP layers 6 and 7 is lower than that of the p-type InP layer 8, the diffusion of Zn from the p-type InP layer 8 as shown in FIG. Layer 6, 7
The growth front that reaches the top of the mesa due to the offset of the upper carriers does not provide an effective current leakage path.

【0016】すると、n−InP電流ブロック層17
(Siドープn型InP層6,7からZnが拡散したI
nP層16を除いた部分)は、後にこの上方に成長する
n型InP層9又は10と分離された構造となる。そし
てこのような構造では、メサストライプの活性領域以外
を流れるリーク電流は効果的に抑止され、低閾値半導体
レーザが実現できる。
Then, the n-InP current blocking layer 17
(I where Zn is diffused from Si-doped n-type InP layers 6 and 7)
The portion excluding the nP layer 16) has a structure that is separated from the n-type InP layer 9 or 10 which grows above the portion later. In such a structure, a leak current flowing in areas other than the active region of the mesa stripe is effectively suppressed, and a low-threshold semiconductor laser can be realized.

【0017】その後SiO2 膜12で電流狭窄を行った
後n電極13を形成、更に基板側を研磨してトータル膜
厚100μm程度にした後p電極14を蒸着により形成
し、素子化を行った。
After that, the current was confined by the SiO 2 film 12, the n-electrode 13 was formed, the substrate side was polished to a total film thickness of about 100 μm, and the p-electrode 14 was formed by vapor deposition to form an element. .

【0018】本実施例によるBHレーザでは、発振波長
1.3μm ,閾電流値10〜12mA,スロ−プ効率
0.3mW/mA の素子が高歩留りで得られ、低リーク
電流で且つ低閾値の半導体レーザが実現できた。
In the BH laser according to the present embodiment, an element having an oscillation wavelength of 1.3 μm, a threshold current value of 10 to 12 mA, and a slope efficiency of 0.3 mW / mA can be obtained at a high yield, a low leakage current and a low threshold voltage. A semiconductor laser has been realized.

【0019】本実施例では半導体レーザへの適用につい
て説明したが、本発明は半導体レーザに限らず電流狭窄
を行う必要のある他のデバイスについても適用可能であ
る。
In this embodiment, the application to a semiconductor laser has been described. However, the present invention is not limited to a semiconductor laser, but can be applied to other devices that need to perform current confinement.

【0020】[0020]

【発明の効果】本発明のように、変曲点の無い滑らかな
側面形状を持つメサストライプをp−n接合により埋め
込む構造で、n−InP電流ブロック層を、第1及び、
第1のキャリア濃度よりも大きい第2のキャリア濃度の
層からなり、この順序で成長する2層構造とし、その後
埋め込むp型InP層のキャリア濃度を上記第2のキャ
リア濃度以上とすれば、ブロック層の成長フロントがメ
サ最上部に達してしまった場合でも、この部分のキャリ
アはその上に成長するp型InP層からのZnの拡散に
より相殺される。そのため、n−n接続が排除でき、リ
ーク電流が小さく、活性領域へ効率的に電流注入を行う
低閾値の素子が得られる。
According to the present invention, a mesa stripe having a smooth side surface shape without an inflection point is buried by a pn junction, and an n-InP current blocking layer is formed by first and second n-InP current blocking layers.
A layer having a second carrier concentration higher than the first carrier concentration and having a two-layer structure grown in this order, and then having a carrier concentration of the p-type InP layer to be buried being equal to or higher than the second carrier concentration, a block is formed. Even if the growth front of the layer reaches the top of the mesa, the carriers in this area are offset by the diffusion of Zn from the overlying p-type InP layer. Therefore, an n-n connection can be eliminated, a leak current is small, and a low-threshold element that efficiently injects current into the active region can be obtained.

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

【図1】本発明の一実施例を示す半導体レーザの断面
図。
FIG. 1 is a sectional view of a semiconductor laser showing one embodiment of the present invention.

【図2】従来例を示す半導体レーザの断面図。FIG. 2 is a sectional view of a semiconductor laser showing a conventional example.

【図3】本発明の一実施例の要部の説明図。FIG. 3 is an explanatory diagram of a main part of one embodiment of the present invention.

【符号の説明】[Explanation of symbols]

1…p−InP基板、2…p−InPクラッド層、3…
MQW活性層、4…n−InPクラッド層、5…p−I
nP層、6…n−InP層、7…Zn拡散p−InP
層、8…p−InP層、9…n−InP層、10…n−
InP層、11…n−InGaAsPキャップ層、12
…SiO2 膜、13…n電極、14…p電極、15…S
iO2 膜、16…Zn拡散InP層、17…n−InP
電流ブロック層。
1 ... p-InP substrate, 2 ... p-InP cladding layer, 3 ...
MQW active layer, 4 ... n-InP cladding layer, 5 ... pI
nP layer, 6 ... n-InP layer, 7 ... Zn diffusion p-InP
Layer, 8 ... p-InP layer, 9 ... n-InP layer, 10 ... n-
InP layer, 11... N-InGaAsP cap layer, 12
... SiO 2 film, 13 ... n electrode, 14 ... p electrode, 15 ... S
iO 2 film, 16 ... Zn diffusion InP layer, 17 ... n-InP
Current block layer.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】半導体基板上に活性層を含む多層構造を形
成し、上記多層構造を、側面が変曲点の無い滑らかな曲
面であるメサストライプ状に加工し、メサ側面を第1導
電型の半導体層及び第2導電型の半導体層を含む半導体
多層膜で埋め込む半導体装置において、最初に上記第1
導電型の半導体層を埋め込み成長し、次に成長する上記
第2導電型の半導体層を、第1及び第2のキャリア濃度
の層からなる2層構造とし、その後さらに第1導電型及
び第2導電型の半導体層により埋め込むことを特徴とす
る半導体レーザ装置。
1. A multi-layered structure including an active layer is formed on a semiconductor substrate, and the multi-layered structure is processed into a mesa stripe shape having a smooth curved surface with no inflection point, and the mesa side surface is formed of a first conductivity type. A semiconductor device embedded with a semiconductor multilayer film including a semiconductor layer of a second conductivity type and a semiconductor layer of a second conductivity type.
The conductive type semiconductor layer is buried and grown, and the second conductive type semiconductor layer to be grown next has a two-layer structure including first and second carrier concentration layers. A semiconductor laser device embedded with a conductive semiconductor layer.
【請求項2】半導体基板上に活性層を含む多層構造を形
成し、該多層構造を、側面が変曲点の無い滑らかな曲面
であるメサストライプ状に加工し、メサ側面を第1導電
型の半導体層及び第2導電型の半導体層を含む半導体多
層膜で埋め込む半導体装置において、最初に第1導電型
の半導体層を埋め込み成長し、次に成長する第2導電型
の半導体層を、第1及び、第1のキャリア濃度よりも大
きい第2のキャリア濃度の層からなり、この順序で成長
する2層構造とし、その後、さらに上記第1導電型及び
上記第2導電型の半導体層により埋め込むことを特徴と
する半導体レーザ装置。
2. A multi-layer structure including an active layer is formed on a semiconductor substrate, and the multi-layer structure is processed into a mesa stripe shape having a smooth curved surface with no inflection points. In the semiconductor device embedded with the semiconductor multilayer film including the semiconductor layer of the second conductivity type and the semiconductor layer of the second conductivity type, the semiconductor layer of the first conductivity type is first embedded and grown, and then the semiconductor layer of the second conductivity type is 1 and a layer having a second carrier concentration higher than the first carrier concentration, and has a two-layer structure grown in this order. Thereafter, the layer is further buried with the semiconductor layers of the first conductivity type and the second conductivity type. A semiconductor laser device characterized by the above-mentioned.
【請求項3】半導体基板上に活性層を含む多層構造を形
成し、該多層構造を、側面が変曲点の無い滑らかな曲面
であるメサストライプ状に加工し、メサ側面を第1導電
型の半導体層及び第2導電型の半導体層を含む半導体多
層膜で埋め込む半導体装置において、最初に第1導電型
の半導体層を埋め込み成長し、次に成長する第2導電型
の半導体層を、第1及び、第1のキャリア濃度よりも大
きい第2のキャリア濃度の層からなり、この順序で成長
する2層構造とし、その後埋め込む上記第1導電型の半
導体層のキャリア濃度を上記第2のキャリア濃度以上と
し、その後さらに上記第2導電型の半導体層により埋め
込むことを特徴とする半導体レーザ装置。
3. A multi-layer structure including an active layer is formed on a semiconductor substrate, and the multi-layer structure is processed into a mesa stripe shape having a smooth curved surface with no inflection point, and the mesa side surface is formed of a first conductivity type. In the semiconductor device embedded with the semiconductor multilayer film including the semiconductor layer of the second conductivity type and the semiconductor layer of the second conductivity type, the semiconductor layer of the first conductivity type is first embedded and grown, and then the semiconductor layer of the second conductivity type is 1 and a layer having a second carrier concentration higher than the first carrier concentration, and has a two-layer structure grown in this order, and thereafter, the carrier concentration of the semiconductor layer of the first conductivity type to be embedded is adjusted to the second carrier concentration. A semiconductor laser device having a concentration equal to or higher than that of the first semiconductor layer and then burying the semiconductor layer with the second conductivity type semiconductor layer.
【請求項4】p型InP基板上に活性層を含む多層構造
を形成し、該多層構造を、側面が変曲点の無い滑らかな
曲面であるメサストライプ状に加工し、メサ側面をZn
ドープp型InP層及びSiドープn型InP層で埋め
込む半導体装置において、最初にp型InP層を埋め込
み成長し、次に成長するn型InP層を、第1及び、第
1のキャリア濃度よりも大きい第2のキャリア濃度の層
からなり、この順序で成長する2層構造とし、その後、
埋め込むp型InP層のキャリア濃度を上記第2のキャ
リア濃度以上とし、その後、さらにn型InP層で埋め
込むことを特徴とする半導体レーザ装置。
4. A multi-layer structure including an active layer is formed on a p-type InP substrate, and the multi-layer structure is processed into a mesa stripe shape having a smooth curved surface without an inflection point, and a mesa side surface formed of Zn.
In a semiconductor device embedded with a doped p-type InP layer and a Si-doped n-type InP layer, a p-type InP layer is first buried and grown, and then the n-type InP layer to be grown has a first carrier concentration lower than the first carrier concentration. A two-layer structure consisting of a layer having a large second carrier concentration and growing in this order;
A semiconductor laser device wherein the carrier concentration of a p-type InP layer to be buried is set to be equal to or higher than the second carrier concentration, and then the n-type InP layer is further buried.
JP01094897A 1997-01-24 1997-01-24 Semiconductor laser device Expired - Fee Related JP3877823B2 (en)

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JP01094897A JP3877823B2 (en) 1997-01-24 1997-01-24 Semiconductor laser device

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Application Number Priority Date Filing Date Title
JP01094897A JP3877823B2 (en) 1997-01-24 1997-01-24 Semiconductor laser device

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JPH10209561A true JPH10209561A (en) 1998-08-07
JP3877823B2 JP3877823B2 (en) 2007-02-07

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115023869A (en) * 2020-01-28 2022-09-06 三菱电机株式会社 Optical semiconductor device and method of manufacturing the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115023869A (en) * 2020-01-28 2022-09-06 三菱电机株式会社 Optical semiconductor device and method of manufacturing the same

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