JP2000294883A - Nitride compound semiconductor laser element - Google Patents
Nitride compound semiconductor laser elementInfo
- Publication number
- JP2000294883A JP2000294883A JP11097903A JP9790399A JP2000294883A JP 2000294883 A JP2000294883 A JP 2000294883A JP 11097903 A JP11097903 A JP 11097903A JP 9790399 A JP9790399 A JP 9790399A JP 2000294883 A JP2000294883 A JP 2000294883A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- type
- compound semiconductor
- thickness
- semiconductor laser
- 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
Links
- 239000004065 semiconductor Substances 0.000 title claims abstract description 52
- -1 Nitride compound Chemical class 0.000 title claims abstract description 5
- 238000005253 cladding Methods 0.000 claims description 29
- 150000001875 compounds Chemical class 0.000 claims description 29
- 150000004767 nitrides Chemical class 0.000 claims description 25
- 238000000034 method Methods 0.000 claims description 19
- 238000004519 manufacturing process Methods 0.000 claims description 11
- 239000000463 material Substances 0.000 claims description 7
- 239000000758 substrate Substances 0.000 abstract description 44
- 229910002704 AlGaN Inorganic materials 0.000 abstract description 14
- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 abstract description 10
- 125000005842 heteroatom Chemical group 0.000 abstract 3
- 230000003287 optical effect Effects 0.000 description 20
- 238000002488 metal-organic chemical vapour deposition Methods 0.000 description 14
- 229910052710 silicon Inorganic materials 0.000 description 12
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 11
- 238000009826 distribution Methods 0.000 description 11
- 239000010703 silicon Substances 0.000 description 11
- 230000004888 barrier function Effects 0.000 description 7
- 238000001312 dry etching Methods 0.000 description 7
- 229910052594 sapphire Inorganic materials 0.000 description 7
- 239000010980 sapphire Substances 0.000 description 7
- 238000009834 vaporization Methods 0.000 description 5
- 230000008016 vaporization Effects 0.000 description 5
- 229910004298 SiO 2 Inorganic materials 0.000 description 4
- 239000000969 carrier Substances 0.000 description 3
- 238000007796 conventional method Methods 0.000 description 3
- 230000010355 oscillation Effects 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000001704 evaporation Methods 0.000 description 2
- 238000001816 cooling Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 238000007687 exposure technique Methods 0.000 description 1
- 230000017525 heat dissipation Effects 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 230000000644 propagated effect Effects 0.000 description 1
- 230000001681 protective effect Effects 0.000 description 1
Landscapes
- Semiconductor Lasers (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、窒化物系化合物半
導体(InXAlYGa1-X-YN、X≧0、Y≧0、X+Y≦1)レーザ素子
の製造方法と、該製造方法を用いて作製された、窒化物
系化合物半導体(InXAlYGa1-X-YN、X≧0、Y≧0、X+Y≦1)
レーザ素子に関する。The present invention relates to a method for manufacturing a nitride-based compound semiconductor (In X Al Y Ga 1 -XYN , X ≧ 0, Y ≧ 0, X + Y ≦ 1) laser device, and a method for manufacturing the same. Prepared using the method, nitride-based compound semiconductor (In X Al Y Ga 1-XYN , X ≧ 0, Y ≧ 0, X + Y ≦ 1)
The present invention relates to a laser device.
【0002】[0002]
【従来の技術】従来作製された窒化物系化合物半導体レ
ーザのストライプ幅方向の光や電流を閉じ込める方法
は、アプライド・フィジックス・レターズ(APPLIED PH
YSISCSLETTERS) 第68巻 3269頁 1996年
に記載されているような利得導波型ストライプレーザ
や、アプライド・フィジックス・レターズ(APPLIED PH
YSISCS LETTERS) 第69巻 1477頁 1996年
に記載されているようなリッジ構造や特開平9−246
763号に記載されているようなクラッド層埋め込み型
レーザなどがあり、我々も図8のようなリッジ型レーザ
で室温連続発振を実現した。図8は、従来の技術で作製
された代表的なリッジ構造レーザの断面構造である。n
型GaN基板101上にSiドープn型Al0.1Ga0.9N(シ
リコン濃度4×1017 atoms/cm3、厚さ1μm)から
なるn型クラッド層102、 Siドープn型GaN(シリ
コン濃度4×1017 atoms/cm3、厚さ0.1μm)からな
るn型光閉じ込め層103、 In0.2Ga0.8N(厚さ3n
m)井戸層とIn0.05Ga0.95N (厚さ5nm)バリア層からな
るアンドープMQW活性層104(井戸数3個)、Mgドー
プp型Al0.2Ga0.8N からなるキャップ層105、Mgドー
プp型GaN(Mg濃度2×101 7 atoms/cm3、厚さ0.1μ
m)からなるp型光閉じ込め層106、Mgドープp型Al0
.1Ga0.9N(Mg濃度2×1017 atoms/cm3、厚さ0.5μ
m)からなるp型クラッド層107、Mgドープp型GaN(M
g濃度2×1017 atoms/cm3、厚さ0.1μm)からなる
p型コンタクト層108を順次成長させて、レーザーダ
イオード構造(以下LD構造と記す。)を形成する。レー
ザ構造はMOCVD装置で成長が行われ、成長温度は、InGaN
MQW活性層104は780℃であり、その他の層はす
べて1050℃で行った。ドライエッチングによりp型
クラッド層107そしてp型コンタクト層108を含ん
だメサ型109を部分的に残した後、SiO2絶縁膜110
をつけ、メサ部分の頭出しを露光技術により行い、リッ
ジ構造を形成した。n型基板裏にはTi/Alからなるn電
極111を形成し、pコンタクト上には、Ni/Auからなる
p電極112を形成した。2. Description of the Related Art Conventionally, a method for confining light and current in a stripe width direction of a nitride-based compound semiconductor laser is disclosed in Applied Physics Letters.
YSISCSLETTERS) Vol. 68, p. 3269, 1996
Gain-guided stripe lasers such as those described in Applied Physics Letters (APPLIED PH
YSISCS LETTERS) Vol. 69, p. 1,477. Ridge structure as described in 1996 or JP-A-9-246.
No. 763, there is a laser with a buried cladding layer, and the like, and we have also realized continuous oscillation at room temperature with a ridge type laser as shown in FIG. FIG. 8 shows a cross-sectional structure of a typical ridge structure laser manufactured by a conventional technique. n
An n-type clad layer 102 made of Si-doped n-type Al 0.1 Ga 0.9 N (silicon concentration 4 × 10 17 atoms / cm 3 , thickness 1 μm) on a Si-type n-type GaN (silicon concentration 4 × 10 N-type optical confinement layer 103 of 17 atoms / cm 3 , 0.1 μm in thickness, In 0.2 Ga 0.8 N (thickness 3 n
m) Undoped MQW active layer 104 (three wells) composed of a well layer and an In 0.05 Ga 0.95 N (thickness 5 nm) barrier layer, cap layer 105 composed of Mg-doped p-type Al 0.2 Ga 0.8 N, Mg-doped p-type GaN (Mg concentration 2 × 10 1 7 atoms / cm 3, a thickness of 0.1μ
m), a p-type optical confinement layer 106 composed of Mg-doped p-type Al 0
.1 Ga 0.9 N (Mg concentration 2 × 10 17 atoms / cm 3 , thickness 0.5μ)
m), a Mg-doped p-type GaN (M
g concentration 2 × 10 17 atoms / cm 3 , thickness 0.1 μm)
A p-type contact layer 108 is sequentially grown to form a laser diode structure (hereinafter, referred to as an LD structure). The laser structure is grown by MOCVD equipment and the growth temperature is InGaN
The MQW active layer 104 was at 780 ° C., and all other layers were at 1050 ° C. After partially leaving the mesa 109 including the p-type cladding layer 107 and the p-type contact layer 108 by dry etching, the SiO 2 insulating film 110 is formed.
Then, the ridge structure was formed by exposing the mesa portion to the crest by an exposure technique. An n-electrode 111 made of Ti / Al was formed on the back of the n-type substrate, and a p-electrode 112 made of Ni / Au was formed on the p-contact.
【0003】[0003]
【発明が解決しようとする課題】しかし、上述したよう
な窒化物系化合物半導体レーザ素子は、横方向に実屈折
率段差のない利得導波型であったり、平坦な活性層と凸
部をもつクラッド層から形成され、凸部に光波が閉じ込
められ伝播するリッジやクラッド層埋め込み構造を有し
ていた。このような構造のレーザは、ストライプ幅方向
の利得分布領域が屈折率分布領域に比べ広く、レーザ発
振に寄与しない余分なキャリアが損失されるのでしきい
値電流が高くなり、高出力化していくとストライプ外
(導波路外部)の利得が上昇し、ストライプ内外での実
効屈折率差が減少するために横モードの安定性が悪くな
る。また、p電極側から放熱を行いたい場合、活性領域
がSiO2等の絶縁物で埋め込まれていたので熱伝導性
が悪くなり、素子の温度上昇により素子寿命を短くする
欠点があった。これらの問題を解決するためには、スト
ライプ幅方向の利得領域と屈折率分布領域が一致する構
造を作製する必要があり、その手法として活性層を含む
メサ型高屈折率領域(導波路)を低屈折率半導体を再成
長し活性層を埋め込んだレーザ構造が提案されている
(特開平8-330678等)。しかし、本発明者の検討によれ
ば、この手法を用いるとInGaNを活性層とする窒化物系
半導体レーザでは、製造工程中における低い温度で成長
される活性層が比較的高温で行われる埋め込み層の成長
時に高温にさらされ、活性層内部で原子配列が乱れた
り、活性層から原子が気化するなどの問題点があること
が判明した。そこで本発明の目的は上記の問題点を解決
し、しきい値電流が低く、横モードが安定しており、寿
命の長い窒化物系化合物半導体レーザ素子を提供するこ
とである。However, the above-mentioned nitride-based compound semiconductor laser device is of a gain waveguide type having no actual refractive index step in the lateral direction, or has a flat active layer and a convex portion. It had a ridge or cladding layer buried structure formed of a cladding layer, in which light waves were confined and propagated in the projections. In a laser having such a structure, the gain distribution region in the stripe width direction is wider than the refractive index distribution region, and extra carriers that do not contribute to laser oscillation are lost, so that the threshold current increases and the output increases. Then, the gain outside the stripe (outside the waveguide) increases, and the difference in effective refractive index inside and outside the stripe decreases, so that the stability of the transverse mode deteriorates. Further, when it is desired to radiate heat from the p-electrode side, since the active region is buried with an insulator such as SiO 2, thermal conductivity is deteriorated, and there is a disadvantage that the life of the device is shortened due to a rise in temperature of the device. In order to solve these problems, it is necessary to fabricate a structure in which the gain region and the refractive index distribution region in the stripe width direction coincide with each other. As a technique, a mesa-type high refractive index region (waveguide) including an active layer is used. A laser structure in which a low-refractive index semiconductor is regrown and an active layer is buried has been proposed (JP-A-8-330678). However, according to the study of the present inventor, using this method, in a nitride semiconductor laser using InGaN as an active layer, an active layer grown at a low temperature during the manufacturing process is a buried layer which is formed at a relatively high temperature. It has been found that there are problems such as the atomic arrangement being disordered inside the active layer and the vaporization of atoms from the active layer due to exposure to high temperatures during the growth of. SUMMARY OF THE INVENTION An object of the present invention is to solve the above problems and to provide a nitride-based compound semiconductor laser device having a low threshold current, a stable transverse mode, and a long life.
【0004】[0004]
【問題を解決するための手段】本発明は、基板上部に形
成されたInXGa1-XN(0≦X≦1)からなる活性層と、該活
性層の上側に存在する第一のクラッド層の双方ともがメ
サ型ストライプ構造中に存在しており、該メサ型ストラ
イプ構造の側面に、活性層よりも低屈折率の半導体から
なる埋込み層が存在する窒化物系化合物半導体レーザー
素子の製造方法において、前記活性領域の成長温度より
も100℃高い温度以下の温度で埋め込み層を成長する
ことを特徴とする窒化物系化合物半導体レーザー素子の
製造方法。According to the present invention, there is provided an active layer comprising In X Ga 1 -X N (0 ≦ X ≦ 1) formed on a substrate, Both of the cladding layers are present in the mesa-type stripe structure, and a nitride-based compound semiconductor laser device in which a buried layer made of a semiconductor having a lower refractive index than the active layer is present on the side surface of the mesa-type stripe structure. The method of manufacturing a nitride-based compound semiconductor laser device, wherein the buried layer is grown at a temperature not higher than 100 ° C. higher than the growth temperature of the active region.
【0005】上述したように、従来、埋め込み層の成長
温度は活性層の成長温度よりも高温である事が多く、活
性層中の原子配列を乱したり、活性層からの原子の気化
を引き起こすなど、活性層の品質を劣化させる原因とな
っていた。しかし、本発明では、活性層の成長温度以下
で埋め込み層の成長を行うことで、活性層の劣化を引き
起こすことなく、埋込み層を形成することが可能となっ
た。As described above, conventionally, the growth temperature of the buried layer is often higher than the growth temperature of the active layer, which disturbs the arrangement of atoms in the active layer and causes vaporization of atoms from the active layer. For example, it causes the quality of the active layer to deteriorate. However, in the present invention, the buried layer can be formed without causing deterioration of the active layer by growing the buried layer at a temperature lower than the growth temperature of the active layer.
【0006】埋め込み層の成長は、活性層の成長温度よ
りも100℃高い温度以下の温度で行われるが、好まし
くは活性層の成長温度よりも50℃高い温度以下の温度
であり、最も好ましくは活性層の成長温度以下で行われ
る。The buried layer is grown at a temperature not higher than 100 ° C. higher than the growth temperature of the active layer, preferably at a temperature not higher than 50 ° C. higher than the growth temperature of the active layer, and most preferably. This is performed at a temperature lower than the growth temperature of the active layer.
【0007】前記、埋込み層の材料としてはII-VI族化
合物半導体を用いることができる。例えば、MgSeは325
℃と非常に低い温度で成長することが可能であり、活性
層を高温から保護することができる。As the material of the buried layer, a II-VI group compound semiconductor can be used. For example, MgSe is 325
It is possible to grow at a very low temperature of ° C. and to protect the active layer from high temperatures.
【0008】また、埋め込み層としてInXAlYGa1-X-YN
(X≧0、Y≧0、X+Y≦1)の組成の窒化化合物半導体を材
料とすることも可能である。また、埋め込み層を多層膜
とすることも可能である。この場合は、埋め込み層中に
逆バイアス構造を形成することで、素子のリーク電流を
減少することが可能となるとともに、素子の耐電圧特性
を向上することできる。[0008] Further, In X Al Y Ga 1-XY N
It is also possible to use a nitride compound semiconductor having a composition of (X ≧ 0, Y ≧ 0, X + Y ≦ 1) as a material. Also, the buried layer can be a multilayer film. In this case, by forming a reverse bias structure in the buried layer, it is possible to reduce the leak current of the device and to improve the withstand voltage characteristics of the device.
【0009】また、埋め込み層を多層膜とした場合、II
−VI族化合物半導体とInXAlYGa1-X- YN(X≧0、Y≧0、X+
Y≦1)の両者を組み合わせて多層膜とすることも可能で
ある。When the buried layer is a multilayer film,
-VI compound semiconductor and In X Al Y Ga 1-X- Y N (X ≧ 0, Y ≧ 0, X +
Y ≦ 1) may be combined to form a multilayer film.
【0010】また、第一の埋め込み層を活性層の成長温
度以下の温度で前記メサ型ストライプ構造の表面に薄く
成長し、その後、温度を活性層の成長温度以上に上昇
し、引き続き第二の埋め込み層を再成長することも可能
である。この場合、最初に成長された薄い埋め込み層
は、活性層表面から気化により原子が失われるのを防ぐ
ための保護膜として機能する。A first buried layer is grown thinly on the surface of the mesa-type stripe structure at a temperature lower than the growth temperature of the active layer, and then the temperature is raised to a temperature higher than the growth temperature of the active layer. It is also possible to regrow the buried layer. In this case, the thin buried layer grown first functions as a protective film for preventing atoms from being lost from the surface of the active layer due to vaporization.
【0011】前記、「薄く成長する」とは、活性層の成
長温度以上の高温で行われる前記第二の埋め込み層の成
長時に、活性層から原子の気化を抑制するに足るだけの
膜厚を成長することである。具体的には、材料としてIn
0.1Ga0.9Nを用いた場合には5Å〜1000Åの膜厚で
ある事が好ましい。[0011] The term "grow thinly" means that when the second buried layer is grown at a temperature higher than the growth temperature of the active layer, a film thickness sufficient to suppress the vaporization of atoms from the active layer. It is to grow. Specifically, the material is In
When 0.1 Ga 0.9 N is used, the film thickness is preferably 5 to 1000 °.
【0012】また、以上の方法を用いて作製された高品
質の窒化物系化合物半導体レーザー素子を提供する。Further, there is provided a high-quality nitride-based compound semiconductor laser device manufactured by using the above method.
【0013】[0013]
【発明の実施の形態】本発明の実施形態について、実施
例に基づき図面を参照して詳細に説明する。 (実施例1)図1は実施例である半導体レーザの構造断
面図である。本例では、埋め込み層を活性層の成長温度
以下の温度で再成長させることで活性層の保護を行って
いる。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Embodiments of the present invention will be described in detail based on embodiments with reference to the drawings. (Embodiment 1) FIG. 1 is a structural sectional view of a semiconductor laser according to an embodiment. In this example, the active layer is protected by regrowing the buried layer at a temperature lower than the growth temperature of the active layer.
【0014】n型GaN基板1上にSiドープn型Al0.1G
a0.9N(シリコン濃度4×1017atoms/cm3、厚さ1μ
m)からなるn型クラッド層2、Siドープn型GaN(シ
リコン濃度4×1017atoms/cm3、厚さ0.1μm)からな
るn型光閉じ込め層3、In0.2Ga0.8N(厚さ3nm)井戸
層とIn0.05Ga0.95N (厚さ5nm)バリア層からなるアンド
ープMQW層4(井戸数3個)、Mgドープp型Al0.2Ga0.8N
(Mg濃度2×1017 atoms/cm3、厚さ20nm)からなる
キャップ層5、Mgドープp型GaN(Mg濃度2×101 7 at
oms/cm3、厚さ0.1μm)からなるp型光閉じ込め層6、
Mgドープp型Al0.1Ga0.9N(Mg濃度2×1017 atoms/
cm3、厚さ0.5μm)からなるp型クラッド層7、 Mgド
ープp型GaN(Mg濃度2×1017 atoms/cm3、厚さ0.2
μm)からなるp型コンタクト層8を順次成長させて、L
D構造を形成する。レーザ構造はMOCVD装置で成長が行わ
れ、成長温度は、InGaN MQW活性層4は780℃であ
り、その他の層はすべて1050℃で行う。ドライエッ
チングによりMQW活性層4、p型光閉じ込め層6、p型ク
ラッド層7そしてp型コンタクト層8を含んだメサ型9
を部分的に残した後、MOCVD法の再成長により成長温度
780℃でアンドープAl0.2Ga0.8N(厚さ0.75μm)埋
め込み層10を形成した。n型基板裏にはTi/Alからな
るn電極11を形成し、pコンタクト上には、Ni/Auから
なるp電極12を形成する。On an n-type GaN substrate 1, Si-doped n-type Al 0.1 G
a 0.9 N (silicon concentration 4 × 10 17 atoms / cm 3 , thickness 1μ)
m), an n-type optical confinement layer 3 made of Si-doped n-type GaN (silicon concentration 4 × 10 17 atoms / cm 3 , thickness 0.1 μm), In 0.2 Ga 0.8 N (thickness 3 nm) ) Undoped MQW layer 4 (three wells) composed of well layer and In 0.05 Ga 0.95 N (5 nm thick) barrier layer, Mg-doped p-type Al 0.2 Ga 0.8 N
(Mg concentration 2 × 10 17 atoms / cm 3 , thickness 20 nm) cap layer 5 made of, Mg-doped p-type GaN (Mg concentration 2 × 10 1 7 at
oms / cm 3 , 0.1 μm thick)
Mg-doped p-type Al 0.1 Ga 0.9 N (Mg concentration 2 × 10 17 atoms /
a p-type cladding layer 7 of cm 3 and a thickness of 0.5 μm; Mg-doped p-type GaN (Mg concentration: 2 × 10 17 atoms / cm 3 ; thickness: 0.2)
.mu.m), and a p-type contact layer 8 of
Form a D structure. The laser structure is grown in a MOCVD apparatus, and the growth temperature is 780 ° C. for the InGaN MQW active layer 4 and 1050 ° C. for all other layers. Mesa type 9 including MQW active layer 4, p-type optical confinement layer 6, p-type cladding layer 7, and p-type contact layer 8 by dry etching
Was partially left, and an undoped Al 0.2 Ga 0.8 N (0.75 μm thick) buried layer 10 was formed at a growth temperature of 780 ° C. by regrowth by MOCVD. An n-electrode 11 made of Ti / Al is formed on the back of the n-type substrate, and a p-electrode 12 made of Ni / Au is formed on the p-contact.
【0015】n型GaN基板を用いたが、AlGaN基板でもSi
C基板でもサファイア基板などを用いてもよく、極性もp
やi型でもよい。また本実施例では埋め込み層9はアン
ドープAlGaNであったが、極性はn型でもよい。Although an n-type GaN substrate is used, an AlGaN substrate
A C substrate or a sapphire substrate may be used.
Or i-type. Further, in this embodiment, the buried layer 9 is undoped AlGaN, but the polarity may be n-type.
【0016】また、埋め込み材料もInXAlYGa1-X-YN(X
≧0、Y≧0、X+Y≦1)でもよい。The filling material is also In X Al Y Ga 1-XY N (X
≧ 0, Y ≧ 0, X + Y ≦ 1).
【0017】(実施例2)図2は実施例である半導体レ
ーザの構造断面図である。(Embodiment 2) FIG. 2 is a structural sectional view of a semiconductor laser according to an embodiment.
【0018】p型 Al0.1Ga0.9N基板13上にMgドー
プp型Al0.1Ga0.9N(Mg濃度2×1017 atoms/cm3、
厚さ1μm)からなるp型クラッド層14、 Mgドー
プp型GaN(Mg濃度2×1017 atoms/cm3、厚さ0.1
μm)からなるp型光閉じ込め層15、Siドープ In
0.2Ga0.8N(Si濃度2×1017 atoms/cm3、厚さ3nm)
井戸層とIn0.05Ga0.95N (厚さ5nm)バリア層からなるS
iドープMQW層16(井戸数3個)Siドープp型Al0.2Ga
0.8N(Si濃度2×1017 atoms/cm3、厚さ20nm)から
なるキャップ層17、Siドープn型GaN(Si濃度4×1
017 atoms/cm3、厚さ0.1μm)からなるn型光閉じ込
め層18、 Siドープn型Al0.1Ga0.9N(Si濃度4×1
017 atoms/cm3、厚さ2μm)からなるn型クラッド層
19、 Siドープn型GaN(Si濃度8×1018atoms/c
m3、厚さ0.05μm)からなるn型コンタクト層20
を順次成長させて、LD構造を形成する。レーザ構造はMO
CVD装置で成長が行われ、成長温度は、InGaN MQW活性
層16は780℃であり、その他の層はすべて1050
℃で行う。ドライエッチングによりMQW活性層16、n
型光閉じ込め層18、p型クラッド層19そしてp型コ
ンタクト層20を含んだメサ型21を部分的に残した
後、MOCVD法の再成長により成長温度780℃でSiドー
プn型Al0.2Ga0.8N(Si濃度7×1017 atoms/cm3、厚
さ0.5μm)埋め込み層22、Mgドープp型Al0.2Ga0.8N
(Mg濃度2×1017 atoms/cm3、厚さ0.5μm)埋め
込み層23、Siドープn型Al0.2Ga0.8N(Si濃度7×1
017 atoms/cm3、厚さ1.2μm)埋め込み層24を
形成する。p型基板裏にはNi/Auからなるp電極25を
形成し、nコンタクト上には、Ti/Al からなるn電極
26を形成する。本実施例では、p型AlGaN基板を用い
たが、GaN基板でもSiC基板でもサファイア基板などを用
いてもよく、極性もnやi型でもよい。[0018] p-type Al 0.1 Ga 0.9 N Mg-doped on the substrate 13 p-type Al 0.1 Ga 0.9 N (Mg concentration 2 × 10 17 atoms / cm 3 ,
A p-type cladding layer 14 of 1 μm thickness, Mg-doped p-type GaN (Mg concentration 2 × 10 17 atoms / cm 3 , thickness 0.1
μm), a p-type optical confinement layer 15, Si-doped In
0.2 Ga 0.8 N (Si concentration 2 × 10 17 atoms / cm 3 , thickness 3 nm)
S consisting of a well layer and an In 0.05 Ga 0.95 N (5 nm thick) barrier layer
i-doped MQW layer 16 (three wells) Si-doped p-type Al 0.2 Ga
A cap layer 17 of 0.8 N (Si concentration 2 × 10 17 atoms / cm 3 , thickness 20 nm), Si-doped n-type GaN (Si concentration 4 × 1
N-type optical confinement layer 18 made of 0 17 atoms / cm 3 and 0.1 μm in thickness; Si-doped n-type Al 0.1 Ga 0.9 N (Si concentration 4 × 1
N-type cladding layer 19 composed of 0 17 atoms / cm 3 and 2 μm in thickness; Si-doped n-type GaN (Si concentration: 8 × 10 18 atoms / c)
m 3 , thickness 0.05 μm)
Are sequentially grown to form an LD structure. Laser structure is MO
The growth is performed in a CVD apparatus. The growth temperature is 780 ° C. for the InGaN MQW active layer 16 and 1050 for all other layers.
Perform at ° C. MQW active layer 16, n by dry etching
After partially leaving the mesa 21 including the p-type optical confinement layer 18, the p-type cladding layer 19 and the p-type contact layer 20, the Si-doped n-type Al 0.2 Ga 0.8 at a growth temperature of 780 ° C. by MOCVD. N (Si concentration 7 × 10 17 atoms / cm 3 , thickness 0.5 μm) buried layer 22, Mg-doped p-type Al 0.2 Ga 0.8 N
(Mg concentration 2 × 10 17 atoms / cm 3 , thickness 0.5 μm) buried layer 23, Si-doped n-type Al 0.2 Ga 0.8 N (Si concentration 7 × 1
(0 17 atoms / cm 3 , thickness 1.2 μm) The buried layer 24 is formed. A p-electrode 25 made of Ni / Au is formed on the back of the p-type substrate, and an n-electrode 26 made of Ti / Al is formed on the n-contact. In this embodiment, a p-type AlGaN substrate is used, but a GaN substrate, a SiC substrate, a sapphire substrate, or the like may be used, and the polarity may be n-type or i-type.
【0019】本実施例では、埋め込み層を3層としてい
る。これは、埋め込み層中に逆バイアス構造を導入する
ためである。埋め込み層中に導入された逆バイアス構造
により、素子のリーク電流が減少するとともに、素子の
耐電圧特性が向上する。In this embodiment, there are three buried layers. This is to introduce a reverse bias structure in the buried layer. The reverse bias structure introduced into the buried layer reduces the leak current of the device and improves the withstand voltage characteristics of the device.
【0020】(実施例3)図3は実施例である半導体レ
ーザの構造断面図である。(Embodiment 3) FIG. 3 is a structural sectional view of a semiconductor laser according to an embodiment.
【0021】本実施例では埋め込み層を2層に分けて再
成長することで、活性層の保護を行っている。n型Al
0.1Ga0.9N基板27上にSiドープn型Al0.1Ga0.9N(シリ
コン濃度4×101 7 atoms/cm3、厚さ1μm)からなる
n型クラッド層28、 Siドープn型GaN(シリコン濃
度4×1017 atoms/cm3、厚さ0.1μm)からなるn型
光閉じ込め層29、 In0.2Ga0.8N(厚さ3nm)井戸層
とIn0.05Ga0.95N (厚さ5nm)バリア層からなるアンドー
プMQW層30(井戸数3個)、Mgドープp型Al0.2Ga0.8N
(Mg濃度2×1017 atoms/cm3、厚さ20nm)からなる
キャップ層31、Mgドープp型GaN(Mg濃度2×1017 a
toms/cm3、厚さ0.1μm)からなるp型光閉じ込め層3
2、Mgドープp型Al0.1Ga0.9N(Mg濃度2×1017 atoms
/cm3、厚さ2μm)からなるp型クラッド層33、Mgド
ープp型GaN(Mg濃度2×1017 atoms/cm3、厚さ0.0
5μm)からなるp型コンタクト層34を順次成長させ
て、LD構造を形成する。レーザ構造はMOCVD装置で成長
が行われ、成長温度は、InGaN MQW活性層30は780
℃であり、その他の層はすべて1050℃で行う。ドラ
イエッチングによりMQW活性層30、p型光閉じ込め層3
2、p型クラッド層33そしてp型コンタクト層34を
含んだメサ型35を部分的に残した後、MOCVD法の再成
長により成長温度780℃でアンドープIn0.05Ga0.95N
(厚さ0.1μm)埋め込み層36、続いてアンドープAl0.2
Ga0.8N(厚さ0.75μm)埋め込み層37を形成する。こ
こで、 In0.05Ga0.95Nを第一層の埋め込み層としたの
は、低温でも良質の膜を成長可能だからである。n型基
板裏にはTi/Alからなるn電極38を形成し、pコンタ
クト31上には、Ni/Auからなるp電極39を形成す
る。本実施例では、n型AlGaN基板を用いたが、GaN基板
でもSiC基板でもサファイア基板などを用いてもよく、
極性もpやi型でもよい。In this embodiment, the active layer is protected by dividing the buried layer into two layers and growing again. n-type Al
0.1 Ga 0.9 N Si on the substrate 27 doped n-type Al 0.1 Ga 0.9 N (silicon concentration 4 × 10 1 7 atoms / cm 3, a thickness of 1 [mu] m) n-type cladding layer 28 made of, Si-doped n-type GaN (silicon concentration An n-type optical confinement layer 29 of 4 × 10 17 atoms / cm 3 and a thickness of 0.1 μm, an In 0.2 Ga 0.8 N (thickness of 3 nm) well layer and an In 0.05 Ga 0.95 N (thickness of 5 nm) barrier layer Undoped MQW layer 30 (three wells), Mg-doped p-type Al 0.2 Ga 0.8 N
(Mg concentration 2 × 10 17 atoms / cm 3 , thickness 20 nm), a cap layer 31 made of Mg-doped p-type GaN (Mg concentration 2 × 10 17 a
p-type optical confinement layer 3 consisting of toms / cm 3 and thickness of 0.1 μm)
2. Mg-doped p-type Al 0.1 Ga 0.9 N (Mg concentration 2 × 10 17 atoms
/ cm 3 , 2 μm thick) p-type cladding layer 33, Mg-doped p-type GaN (Mg concentration 2 × 10 17 atoms / cm 3 , thickness 0.0
An LD structure is formed by sequentially growing a p-type contact layer 34 of 5 μm). The laser structure was grown in a MOCVD apparatus, and the growth temperature was 780 for the InGaN MQW active layer 30.
C., and all other layers are performed at 1050.degree. MQW active layer 30 and p-type optical confinement layer 3 by dry etching
2. After partially leaving the mesa 35 including the p-type cladding layer 33 and the p-type contact layer 34, undoped In 0.05 Ga 0.95 N at a growth temperature of 780 ° C. by regrowth by MOCVD.
(Thickness 0.1 μm) buried layer 36 followed by undoped Al 0.2
A buried layer 37 of Ga 0.8 N (thickness 0.75 μm) is formed. Here, the reason why In 0.05 Ga 0.95 N is used as the first buried layer is that a high quality film can be grown even at a low temperature. An n-electrode 38 made of Ti / Al is formed on the back of the n-type substrate, and a p-electrode 39 made of Ni / Au is formed on the p-contact 31. In this embodiment, an n-type AlGaN substrate was used, but a GaN substrate, a SiC substrate, a sapphire substrate, or the like may be used.
The polarity may be p or i type.
【0022】(実施例4)図4は実施例である半導体レ
ーザの構造断面図である。(Embodiment 4) FIG. 4 is a structural sectional view of a semiconductor laser according to an embodiment.
【0023】本例では、埋め込み層を活性層の成長温度
以下の温度で再成長させることで活性層の保護を行って
いる。In this embodiment, the active layer is protected by regrowing the buried layer at a temperature lower than the growth temperature of the active layer.
【0024】p型 Al0.1Ga0.90N基板40上にMgドー
プp型Al0.1Ga0.90N(Mg濃度2×1017 atoms/c
m3、厚さ1μm)からなるp型クラッド層41、 Mg
ドープp型GaN(Mg濃度2×1017 atoms/cm3、厚さ
0.1μm)からなるp型光閉じ込め層42、Siドープ
In0.2Ga0.8N(Si濃度2×1017 atoms/cm3、厚さ3n
m)井戸層とIn0.05Ga0.95N (厚さ5nm)バリア層からな
るSiドープMQW層43(井戸数3個)、 Siドープp型
Al0.2Ga0.8N(Si濃度2×1017 atoms/cm3、厚さ20n
m)からなるキャップ層44、Siドープn型GaN(Si濃
度4×1017 atoms/cm3、厚さ0.1μm)からなるn型
光閉じ込め層45、 Siドープn型Al0.1Ga0.9N(Si濃
度4×1017 atoms/cm3、厚さ2μm)からなるn型
クラッド層46、Siドープn型GaN(Si濃度8×1018a
toms/cm3、厚さ0.05μm)からなるn型コンタクト
層47を順次成長させて、LD構造を形成する。レーザ構
造はMOCVD装置で成長が行われ、成長温度は、InGaN MQ
W活性層43は780℃であり、その他の層はすべて1
050℃で行う。ドライエッチングによりMQW活性層4
3、n型光閉じ込め層45、p型クラッド層46そして
p型コンタクト層47を含んだメサ型48を部分的に残
した後、MBE法における再成長により成長温度325℃でア
ンドープMgSe(厚さ2.2μm)埋め込み層49を形成す
る。p型基板裏にはNi/Auからなるp電極50を形成
し、nコンタクト上には、Ti/Al からなるn電極51
を形成する。本実施例では、p型AlGaN基板を用いた
が、GaN基板でもSiC基板でもサファイア基板などを用い
てもよく、極性もnやi型でもよい。また、本実施例で
は、埋め込み層としてII−VI族化合物半導体であるMgSe
を用いたがAl 0.1Ga0.90Nクラッド層より低屈折率の材料
であれば どのようなII−VI族化合物半導体でもよい。
また、本実施例では、再成長膜をMBE法によって形成し
たがMOCVD法でもよい。P-type Al0.1Ga0.90Mg dope on N substrate 40
P-type Al0.1Ga0.90N (Mg concentration 2 × 1017 atoms / c
mThree, A 1 μm thick p-type cladding layer 41, Mg
Doped p-type GaN (Mg concentration 2 × 1017 atoms / cmThree,thickness
0.1 μm), p-type optical confinement layer 42, Si-doped
In0.2Ga0.8N (Si concentration 2 × 1017 atoms / cmThree, Thickness 3n
m) Well layer and In0.05Ga0.95N (5 nm thick)
Si-doped MQW layer 43 (3 wells), Si-doped p-type
Al0.2Ga0.8N (Si concentration 2 × 1017 atoms / cmThree, Thickness 20n
m), a Si-doped n-type GaN (Si concentration
Degree 4 × 1017 atoms / cmThree, Thickness 0.1μm)
Optical confinement layer 45, Si-doped n-type Al0.1Ga0.9N (Si rich
Degree 4 × 1017 atoms / cmThree, Thickness 2 μm)
Cladding layer 46, Si-doped n-type GaN (Si concentration 8 × 1018a
toms / cmThreeN-type contact with thickness of 0.05 μm)
The layer 47 is sequentially grown to form an LD structure. Laser structure
The structure is grown by MOCVD equipment and the growth temperature is InGaN MQ
The temperature of the W active layer 43 is 780 ° C.
Perform at 050 ° C. MQW active layer 4 by dry etching
3, n-type optical confinement layer 45, p-type cladding layer 46, and
The mesa 48 including the p-type contact layer 47 is partially left.
After the growth, the growth temperature was 325 ° C by regrowth in the MBE method.
Undoped MgSe (thickness: 2.2 μm) buried layer 49 is formed.
You. Formation of Ni / Au p-electrode 50 on the back of p-type substrate
On the n-contact, an n-electrode 51 made of Ti / Al
To form In this example, a p-type AlGaN substrate was used.
However, using a sapphire substrate or the like for both GaN and SiC substrates
And the polarity may be n-type or i-type. In this embodiment,
Is MgSe which is a II-VI group compound semiconductor as a buried layer.
Using Al 0.1Ga0.90Material with lower refractive index than N cladding layer
Any II-VI compound semiconductor may be used.
In this embodiment, the regrown film is formed by the MBE method.
However, the MOCVD method may be used.
【0025】(実施例5)図5は実施例である半導体レ
ーザの構造断面図である。p型 Al0.1Ga0.90N基板52
上にMgドープp型Al0.1Ga0.90N(Mg濃度2×1017
atoms/cm3、厚さ1μm)からなるp型クラッド層5
3、 Mgドープp型GaN(Mg濃度2×1017 atoms
/cm3、厚さ0.1μm)からなるp型光閉じ込め層54、
Siドープ In0.2Ga0.8N(Si濃度2×1017 atoms/cm
3、厚さ3nm)井戸層とIn0.05Ga0.95N (厚さ5nm)バリ
ア層からなるSiドープMQW層55(井戸数3個)、 S
iドープp型Al0.2Ga0.8N(Si濃度2×1017 atoms/c
m3、厚さ20nm)からなるキャップ層56、Siドープn
型GaN(Si濃度4×1017 atoms/cm3、厚さ0.1μm)
からなるn型光閉じ込め層57、 Siドープn型Al0.1G
a0.9N(Si濃度4×1017 atoms/cm3、厚さ2μm)か
らなるn型クラッド層58、Siドープn型GaN(Si濃度
8×1018atoms/cm3、厚さ0.05μm)からなるn
型コンタクト層59を順次成長させて、LD構造を形成す
る。レーザ構造はMOCVD装置で成長が行われ、成長温度
は、InGaN MQW活性層55は780℃であり、その他の
層はすべて1050℃で行う。ドライエッチングにより
MQW活性層55、n型光閉じ込め層57、p型クラッド
層58そしてp型コンタクト層59を含んだメサ型60
を部分的に残した後、MOCVD法の再成長により成長温度
780℃でアンドープn型Al0.2Ga0.8N(厚さ0.1μ
m)埋め込み層61を成長させた後、成長温度を105
0℃まで上げてアンドープAl0.2Ga0.8N(厚さ2.1μ
m)埋め込み層62を形成する。低い屈折率を持つ埋込
み層62を比較的高温(1050℃)で成長したのは、
結晶性が高く、膜質の良好な埋め込み層を得るためであ
る。p型基板裏にはNi/Auからなるp電極63を形成
し、nコンタクト上には、Ti/Al からなるn電極64
を形成する。本実施例では、p型AlGaN基板を用いた
が、GaN基板でもSiC基板でもサファイア基板などを用い
てもよく、極性もnやi型でもよい。(Embodiment 5) FIG. 5 is a structural sectional view of a semiconductor laser according to an embodiment. p-type Al 0.1 Ga 0.90 N substrate 52
Mg-doped p-type Al 0.1 Ga 0.90 N (Mg concentration 2 × 10 17
atoms / cm 3 , 1 μm thick) p-type cladding layer 5
3. Mg-doped p-type GaN (Mg concentration 2 × 10 17 atoms
/ cm 3 , a thickness of 0.1 μm).
Si doped In 0.2 Ga 0.8 N (Si concentration 2 × 10 17 atoms / cm
3. Si-doped MQW layer 55 (three wells) composed of a well layer and a barrier layer of In 0.05 Ga 0.95 N (thickness of 3 nm)
i-doped p-type Al 0.2 Ga 0.8 N (Si concentration 2 × 10 17 atoms / c
m 3 , thickness of 20 nm)
Type GaN (Si concentration 4 × 10 17 atoms / cm 3 , thickness 0.1 μm)
N-type optical confinement layer 57 composed of Si, n-type Al 0.1 G
a N-type cladding layer 58 of 0.9 N (Si concentration 4 × 10 17 atoms / cm 3 , thickness 2 μm), Si-doped n-type GaN (Si concentration 8 × 10 18 atoms / cm 3 , thickness 0.05 μm) Consisting of n
The mold contact layer 59 is sequentially grown to form an LD structure. The laser structure is grown in a MOCVD apparatus, and the growth temperature is 780 ° C. for the InGaN MQW active layer 55 and 1050 ° C. for all other layers. By dry etching
Mesa 60 including MQW active layer 55, n-type optical confinement layer 57, p-type cladding layer 58 and p-type contact layer 59
Is partially left, and then undoped n-type Al 0.2 Ga 0.8 N (having a thickness of 0.1 μm) at a growth temperature of 780 ° C. by regrowth of the MOCVD method.
m) After growing the buried layer 61, the growth temperature is set to 105
Raise the temperature to 0 ° C and undoped Al 0.2 Ga 0.8 N (thickness 2.1μ
m) The buried layer 62 is formed. The reason for growing the buried layer 62 having a low refractive index at a relatively high temperature (1050 ° C.) is as follows.
This is for obtaining a buried layer having high crystallinity and good film quality. A p-electrode 63 made of Ni / Au is formed on the back of the p-type substrate, and an n-electrode 64 made of Ti / Al is formed on the n-contact.
To form In this embodiment, a p-type AlGaN substrate is used, but a GaN substrate, a SiC substrate, a sapphire substrate, or the like may be used, and the polarity may be n-type or i-type.
【0026】(実施例6)図6は実施例である半導体レ
ーザの構造断面図である。(Embodiment 6) FIG. 6 is a structural sectional view of a semiconductor laser according to an embodiment.
【0027】n型Al0.1Ga0.9N基板65上にSiドープn
型Al0.1Ga0.9N(シリコン濃度4×1017 atoms/cm3、
厚さ1μm)からなるn型クラッド層66、 Siドープ
n型GaN(シリコン濃度4×1017 atoms/cm3、厚さ0.1
μm)からなるn型光閉じ込め層67、 In0.2Ga0.8N
(厚さ3nm)井戸層とIn0.05Ga0.95N (厚さ5nm)バリア
層からなるアンドープMQW層68(井戸数3個)、Mgド
ープp型Al0.2Ga0.8N(Mg濃度2×1017 atoms/cm3、厚
さ20nm)からなるキャップ層69、 Mgドープp型GaN
(Mg濃度2×1017 atoms/cm3、厚さ0.1μm)からな
るp型光閉じ込め層70、 Mgドープp型Al0.1Ga0.9N(M
g濃度2×1017 atoms/cm3、厚さ2μm)からなるp型
クラッド層71、 Mgドープp型GaN(Mg濃度2×1
017、厚さ0.05μm)からなるp型コンタクト層7
2を順次成長させて、LD構造を形成する。レーザ構造は
MOCVD装置で成長が行われ、成長温度は、InGaN MQW活
性層68は780℃であり、その他の層はすべて105
0℃で行う。ドライエッチングによりMQW活性層68、p
型光閉じ込め層70、p型クラッド層71そしてp型コ
ンタクト層72を含んだメサ型73を部分的に残した
後、MOCVD法の再成長により成長温度780℃でMgドー
プp型In0.05Ga0.95N (Mg濃度2×1017、厚さ0.1μm)
埋め込み層74、続いて成長温度を1050℃に上げて
Siドープn型Al0.2Ga0.8N(シリコン濃度4×1017 at
oms/cm3、厚さ1.0μm)埋め込み層75を形成し、続
いて成長温度1050℃でMgドープp型Al0.2Ga0.8N(Mg
濃度2×1017atoms/cm3、厚さ1.1μm)埋め込み層
76を形成する。ここで、埋め込み層74の膜厚は0.1
μmであり、他の埋め込み層に比べて薄いが、これは、
この埋め込み層74が、引き続いて行われる埋込み層7
5,76の成長で用いられる高温(1050℃)により
活性層表面から原子が気化するのを防ぐためだからであ
る。On an n-type Al 0.1 Ga 0.9 N substrate 65, a Si-doped n
Type Al 0.1 Ga 0.9 N (silicon concentration 4 × 10 17 atoms / cm 3 ,
N-type cladding layer 66 of 1 μm thickness, Si-doped n-type GaN (silicon concentration 4 × 10 17 atoms / cm 3 , thickness 0.1
μm), n-type optical confinement layer 67, In 0.2 Ga 0.8 N
An undoped MQW layer 68 (three wells) consisting of a well layer (thickness 3 nm) and an In 0.05 Ga 0.95 N (thickness 5 nm) barrier layer, Mg-doped p-type Al 0.2 Ga 0.8 N (Mg concentration 2 × 10 17 atoms) / cm 3 , 20 nm thick cap layer 69, Mg-doped p-type GaN
(Mg concentration 2 × 10 17 atoms / cm 3 , thickness 0.1 μm), p-type optical confinement layer 70, Mg-doped p-type Al 0.1 Ga 0.9 N (M
a p-type cladding layer 71 having a g concentration of 2 × 10 17 atoms / cm 3 and a thickness of 2 μm; an Mg-doped p-type GaN (Mg concentration 2 × 1
0 17 , p-type contact layer 7 having a thickness of 0.05 μm)
2 are sequentially grown to form an LD structure. Laser structure
The growth was performed in a MOCVD apparatus, and the growth temperature was 780 ° C. for the InGaN MQW active layer 68, and 105 ° C. for all other layers.
Perform at 0 ° C. MQW active layer 68, p
After partially leaving the mesa 73 including the p-type light confinement layer 70, the p-type cladding layer 71, and the p-type contact layer 72, Mg-doped p-type In 0.05 Ga 0.95 at a growth temperature of 780 ° C. by MOCVD. N (Mg concentration 2 × 10 17, thickness 0.1 μm)
Buried layer 74, followed by increasing the growth temperature to 1050 ° C.
Si-doped n-type Al 0.2 Ga 0.8 N (silicon concentration 4 × 10 17 at
oms / cm 3 , thickness 1.0 μm) buried layer 75 is formed, followed by Mg-doped p-type Al 0.2 Ga 0.8 N (Mg
A concentration of 2 × 10 17 atoms / cm 3 and a thickness of 1.1 μm) is formed. Here, the thickness of the buried layer 74 is 0.1
μm, which is thinner than other buried layers.
This buried layer 74 is used for the buried layer 7 to be subsequently formed.
This is because atoms are prevented from evaporating from the surface of the active layer due to the high temperature (1050 ° C.) used for the growth of 5,76.
【0028】n型基板裏にはTi/Alからなるn電極77
を形成し、pコンタクト上には、Ni/Auからなるp電極
78を形成する。本実施例では、n型AlGaN基板を用い
たが、GaN基板でもSiC基板でもサファイア基板などを用
いてもよく、極性もpやi型でもよい。On the back of the n-type substrate, an n-electrode 77 made of Ti / Al
Is formed, and a p-electrode 78 made of Ni / Au is formed on the p-contact. In this embodiment, an n-type AlGaN substrate is used, but a GaN substrate, a SiC substrate, a sapphire substrate, or the like may be used, and the polarity may be p or i-type.
【0029】本実施例では、埋め込み層を3層としてい
る。これは、埋め込み層中に逆バイアス構造を導入する
ためである。埋め込み層中に導入された逆バイアス構造
により、素子のリーク電流が減少するとともに、素子の
耐電圧特性が向上する。In this embodiment, there are three buried layers. This is to introduce a reverse bias structure in the buried layer. The reverse bias structure introduced into the buried layer reduces the leak current of the device and improves the withstand voltage characteristics of the device.
【0030】(実施例7)図7は実施例である半導体レ
ーザの構造断面図である。n型Al0.1Ga0.9N基板79上
にSiドープn型Al0.1Ga0.9N(シリコン濃度4×101 7
atoms/cm3、厚さ1μm)からなるn型クラッド層8
0、 Siドープn型GaN(シリコン濃度4×1017 atom
s/cm3、厚さ0.1μm)からなるn型光閉じ込め層81、
In0.2Ga0.8N(厚さ3nm)井戸層とIn0.05Ga0.95N
(厚さ5nm)バリア層からなるアンドープMQW層82(井戸
数3個)、Mgドープp型Al0.2Ga0.8N(Mg濃度2×1017
atoms/cm3、厚さ20nm)からなるキャップ層83、
Mgドープp型GaN(Mg濃度2×1017 atoms/cm3、厚さ0.
1μm)からなるp型光閉じ込め層84、 Mgドープp型A
l0.1Ga0.9N(Mg濃度2×1017 atoms/cm3、厚さ2μ
m)からなるp型クラッド層85、 Mgドープp型GaN(M
g濃度2×1017 atoms/cm3、厚さ0.05μm)から
なるp型コンタクト層86を順次成長させて、LD構造を
形成する。レーザ構造はMOCVD装置で成長が行われ、成
長温度は、InGaN MQW活性層82は780℃であり、そ
の他の層はすべて1050℃で行う。ドライエッチング
によりMQW活性層82、p型光閉じ込め層84、p型クラ
ッド層85そしてp型コンタクト層86を含んだメサ型
87を部分的に残した後、MOCVD法の再成長により成長
温度600℃でアンドープIn0.05Ga0.95N (厚さ0.03μm)
の第一の埋込み層(図示せず。)を再成長させる。第一
の埋め込み層の材料は、第二の埋込み層と同じである必
要はなく、再成長温度、気化温度、活性層との屈折率の
違い等を勘案して選択される。また、この第一の埋込み
層は引き続いて行われる高温(1050度)の第二の埋
め込み層形成時に活性層が表面から気化するのを防ぐ目
的で形成される。続いて成長温度を1050℃に上げて
5分間待機し、試料を1050度まで昇温し定温とする
とともに、不要な第一の埋め込み層を気化させる。第一
の埋め込み層が気化し終えたらアンドープAl0.2Ga0.8N
(厚さ2.2μm)を材料とする第二の埋め込み層88
を形成する。n型基板裏にはTi/Alからなるn電極89
を形成し、pコンタクト上には、Ni/Auからなるp電極
90を形成する。本実施例では、n型AlGaN基板を用い
たが、GaN基板でもSiC基板でもサファイア基板などを用
いてもよく、極性もpやi型でもよい。(Embodiment 7) FIG. 7 is a structural sectional view of a semiconductor laser according to an embodiment. n-type Al 0.1 Ga 0.9 N Si doped on the substrate 79 n-type Al 0.1 Ga 0.9 N (silicon concentration 4 × 10 1 7
atoms / cm 3 , 1 μm thick) n-type cladding layer 8
0, Si-doped n-type GaN (silicon concentration 4 × 10 17 atom
s / cm 3 , 0.1 μm in thickness).
In 0.2 Ga 0.8 N (thickness 3 nm) well layer and In 0.05 Ga 0.95 N
(5 nm thick) Undoped MQW layer 82 (three wells) composed of a barrier layer, Mg-doped p-type Al 0.2 Ga 0.8 N (Mg concentration 2 × 10 17
atoms / cm 3 , a thickness of 20 nm)
Mg-doped p-type GaN (Mg concentration 2 × 10 17 atoms / cm 3 , thickness 0.
1 μm) p-type optical confinement layer 84, Mg-doped p-type A
l 0.1 Ga 0.9 N (Mg concentration 2 × 10 17 atoms / cm 3 , thickness 2μ)
m), a p-type cladding layer 85 composed of Mg-doped p-type GaN (M
A p-type contact layer 86 having a g concentration of 2 × 10 17 atoms / cm 3 and a thickness of 0.05 μm) is sequentially grown to form an LD structure. The laser structure is grown in a MOCVD apparatus at a growth temperature of 780 ° C. for the InGaN MQW active layer 82 and 1050 ° C. for all other layers. After partially leaving the mesa 87 including the MQW active layer 82, the p-type optical confinement layer 84, the p-type cladding layer 85 and the p-type contact layer 86 by dry etching, the growth temperature is 600 ° C. by regrowth by MOCVD. Undoped with In 0.05 Ga 0.95 N (0.03 μm thickness)
The first buried layer (not shown) is regrown. The material of the first buried layer does not need to be the same as that of the second buried layer, and is selected in consideration of a regrowth temperature, a vaporization temperature, a refractive index difference from the active layer, and the like. The first buried layer is formed for the purpose of preventing the active layer from evaporating from the surface during the subsequent formation of the second buried layer at a high temperature (1050 ° C.). Subsequently, the growth temperature is raised to 1050 ° C., and the sample is waited for 5 minutes. The temperature of the sample is raised to 1050 ° C. to be a constant temperature, and the unnecessary first burying layer is vaporized. Undoped Al 0.2 Ga 0.8 N when the first buried layer has been vaporized
(Buried layer 88 made of (thickness: 2.2 μm))
To form On the back of the n-type substrate, an n-electrode 89 made of Ti / Al
Is formed, and a p-electrode 90 made of Ni / Au is formed on the p-contact. In this embodiment, an n-type AlGaN substrate is used, but a GaN substrate, a SiC substrate, a sapphire substrate, or the like may be used, and the polarity may be p-type or i-type.
【0031】[0031]
【発明の効果】上述したように、本発明により活性層を
含むメサ型を活性層の成長温度以下の成長温度で活性層
よりも屈折率の低い半導体をメサ型構造を挟み込むよう
に再成長することで高温による活性層の品質の劣化を防
ぐことができる。具体的には以下に記す3つの効果が得
られる。As described above, according to the present invention, a mesa structure including an active layer is regrown at a growth temperature lower than the growth temperature of the active layer so that a semiconductor having a lower refractive index than the active layer sandwiches the mesa structure. This can prevent the quality of the active layer from deteriorating due to the high temperature. Specifically, the following three effects are obtained.
【0032】ストライプ幅方向の屈折率分布と利得分
布を一致させることができ、従来構造の利得分布が広い
構造に比べ、余分なキャリアを減らし、横方向のキャリ
ア閉じ込めの能力が向上することから、低いしきい値の
レーザが得られる。Since the refractive index distribution in the stripe width direction and the gain distribution can be matched, the extra carriers are reduced and the capability of confining the carriers in the lateral direction is improved as compared with the conventional structure having a wide gain distribution. A low threshold laser is obtained.
【0033】従来構造の利得分布が広い構造では、光
出力が増すと発振領域外部の利得が大きくなるのに対
し、ストライプ幅方向の屈折率分布と利得分布を一致さ
せることができる本発明の構造では横モードの安定性が
向上する。In the structure having a wide gain distribution of the conventional structure, the gain outside the oscillation region increases as the optical output increases, while the refractive index distribution in the stripe width direction and the gain distribution can be matched. Thus, the stability of the transverse mode is improved.
【0034】従来法ではメサ型ストライプはSiO2
等の絶縁膜で覆われていたので熱伝導が悪く、充分な冷
却効果が得られなかった。しかし、本発明によれば、活
性領域が半導体で埋め込まれているため、従来法にくら
べて放熱性が良くなり素子の寿命を延ばすことが出来
る。In the conventional method, the mesa stripe is made of SiO 2
, Heat conduction was poor, and a sufficient cooling effect could not be obtained. However, according to the present invention, since the active region is buried with the semiconductor, heat dissipation is improved and the life of the element can be extended as compared with the conventional method.
【0035】このように本発明によると窒化物半導体で
屈折率分布と利得分布を一致させる埋め込みレーザ素子
を作製することが可能となった。本発明により得られた
しきい値が低く、高出力時の横モードの安定性に優れ
た、寿命が長い窒化物系化合物半導体レーザー素子は産
業上の利用価値が大きいと考えられる。As described above, according to the present invention, it is possible to manufacture a buried laser device in which a refractive index distribution and a gain distribution are made to match with a nitride semiconductor. It is considered that the nitride-based compound semiconductor laser device having a low threshold obtained by the present invention, having excellent stability of the transverse mode at the time of high output, and having a long life has a great industrial value.
【図1】第1の実施例の窒化物系化合物半導体レーザー
素子の断面図である。FIG. 1 is a sectional view of a nitride-based compound semiconductor laser device according to a first embodiment.
【図2】第2の実施例の窒化物系化合物半導体レーザー
素子の断面図である。FIG. 2 is a sectional view of a nitride-based compound semiconductor laser device according to a second embodiment.
【図3】第3の実施例の窒化物系化合物半導体レーザー
素子の断面図である。FIG. 3 is a sectional view of a nitride-based compound semiconductor laser device according to a third embodiment.
【図4】第4の実施例の窒化物系化合物半導体レーザー
素子の断面図である。FIG. 4 is a sectional view of a nitride-based compound semiconductor laser device according to a fourth embodiment.
【図5】第5の実施例の窒化物系化合物半導体レーザー
素子の断面図である。FIG. 5 is a sectional view of a nitride-based compound semiconductor laser device according to a fifth embodiment.
【図6】第6の実施例の窒化物系化合物半導体レーザー
素子の断面図である。FIG. 6 is a sectional view of a nitride-based compound semiconductor laser device according to a sixth embodiment.
【図7】第7の実施例の窒化物系化合物半導体レーザー
素子の断面図である。FIG. 7 is a sectional view of a nitride-based compound semiconductor laser device according to a seventh embodiment.
【図8】従来の窒化物系化合物半導体レーザー素子の断
面図である。FIG. 8 is a cross-sectional view of a conventional nitride-based compound semiconductor laser device.
1:n型GaN基板 2、19、28、46,58,66、80、102:n
型クラッド層 3、18、29、45、57、67、81、103:n
型光閉じ込め層 4、16、30、43、55、68、82、104:MQ
W活性層 5、31、69、83、105、:p型キャップ層 6、15、32、42、54、70、84、106:p
型光閉じ込め層 7、14、33、41、53、71、85、107:p
型クラッド層 8、34、72、86、108:p型コンタクト層 9、21、35、48、60、73、87、109:メ
サ型 10、49、88:埋め込み層 11、26、38、51、64、77、89、111:
n電極 12、25、39、50、63、78、90、112:
p電極 13:p型AlGaN基板 17、44、56:n型キャップ層 20、47、59:n型コンタクト層 22、36,61、74:第一の埋め込み層 23、37、62、75:第二の埋め込み層 24、76:第三の埋め込み層 27:n型Al0.1Ga0.9N基板 40:p型AlGaN基板 52:p型AlGaN基板 65:n型AlGaN基板 79:n型AlGaN基板 101:n型GaN基板 110:SiO2絶縁膜1: n-type GaN substrate 2, 19, 28, 46, 58, 66, 80, 102: n
Mold cladding layer 3, 18, 29, 45, 57, 67, 81, 103: n
Light confinement layer 4, 16, 30, 43, 55, 68, 82, 104: MQ
W active layer 5, 31, 69, 83, 105: p-type cap layer 6, 15, 32, 42, 54, 70, 84, 106: p
Mold light confinement layers 7, 14, 33, 41, 53, 71, 85, 107: p
Mold cladding layer 8, 34, 72, 86, 108: p-type contact layer 9, 21, 35, 48, 60, 73, 87, 109: mesa type 10, 49, 88: buried layer 11, 26, 38, 51 , 64, 77, 89, 111:
n-electrode 12, 25, 39, 50, 63, 78, 90, 112:
p electrode 13: p-type AlGaN substrate 17, 44, 56: n-type cap layer 20, 47, 59: n-type contact layer 22, 36, 61, 74: first buried layer 23, 37, 62, 75: Second buried layer 24, 76: Third buried layer 27: n-type Al 0.1 Ga 0.9 N substrate 40: p-type AlGaN substrate 52: p-type AlGaN substrate 65: n-type AlGaN substrate 79: n-type AlGaN substrate 101: n Type GaN substrate 110: SiO 2 insulating film
Claims (7)
≦1)からなる活性層と、該活性層の上側に存在する第
一のクラッド層の双方ともがメサ型ストライプ構造中に
存在しており、該メサ型ストライプ構造の側面に、活性
層よりも低屈折率の半導体からなる埋込み層が存在する
窒化物系化合物半導体レーザー素子の製造方法におい
て、前記活性領域の成長温度よりも100℃高い温度以
下の温度で埋め込み層を成長することを特徴とする窒化
物系化合物半導体レーザー素子の製造方法。An In X Ga 1-X N (0 ≦ X
≦ 1), and both the first cladding layer above the active layer are present in the mesa-type stripe structure, and the side of the mesa-type stripe structure is In the method for manufacturing a nitride-based compound semiconductor laser device having a buried layer made of a semiconductor having a low refractive index, the buried layer is grown at a temperature of 100 ° C. or higher than the growth temperature of the active region. A method for manufacturing a nitride-based compound semiconductor laser device.
体を材料とすることを特徴とする請求項1記載の窒化物
系化合物半導体レーザー素子の製造方法。2. The method according to claim 1, wherein the buried layer is made of a II-VI compound semiconductor.
(X≧0、Y≧0、X+Y≦1)の組成の半導体を材料とするこ
とを特徴とする請求項1記載の窒化物系化合物半導体レ
ーザー素子の製造方法。3. An In X Al Y Ga 1-XYN as said buried layer.
2. The method for manufacturing a nitride-based compound semiconductor laser device according to claim 1, wherein a semiconductor having a composition of (X≥0, Y≥0, X + Y≤1) is used as a material.
徴とする請求項1〜3記載の窒化物系化合物半導体レー
ザー素子の製造方法。4. The method for manufacturing a nitride-based compound semiconductor laser device according to claim 1, wherein said buried layer is a multilayer film.
とInXAlYGa1-X-YN(X≧0、Y≧0、X+Y≦1)の両者を材料
として用いたことを特徴とする請求項4記載の窒化物系
化合物半導体レーザー素子の製造方法。5. The semiconductor device according to claim 1, wherein both the II-VI group compound semiconductor and In X Al Y Ga 1-XY N (X ≧ 0, Y ≧ 0, X + Y ≦ 1) are used as the multilayer film. The method for manufacturing a nitride-based compound semiconductor laser device according to claim 4.
の温度で前記メサ型ストライプ構造の表面に薄く成長
し、その後、温度を活性層の成長温度以上に上昇し、引
き続き第二の埋め込み層を再成長することを特徴とする
請求項4に記載の窒化物系化合物半導体レーザー素子の
製造方法。6. A first buried layer is grown thinly on the surface of the mesa-type stripe structure at a temperature equal to or lower than the growth temperature of the active layer, and then the temperature is increased to a temperature equal to or higher than the growth temperature of the active layer. The method for manufacturing a nitride-based compound semiconductor laser device according to claim 4, wherein the buried layer is grown again.
の方法により製造された窒化物系化合物半導体レーザー
素子。7. A nitride compound semiconductor laser device manufactured by the method according to claim 1. Description:
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