JPS6354236B2 - - Google Patents
Info
- Publication number
- JPS6354236B2 JPS6354236B2 JP58085886A JP8588683A JPS6354236B2 JP S6354236 B2 JPS6354236 B2 JP S6354236B2 JP 58085886 A JP58085886 A JP 58085886A JP 8588683 A JP8588683 A JP 8588683A JP S6354236 B2 JPS6354236 B2 JP S6354236B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- optical waveguide
- temperature
- diffraction grating
- active layer
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 230000003287 optical effect Effects 0.000 claims description 18
- 238000000034 method Methods 0.000 claims description 13
- 239000000758 substrate Substances 0.000 claims description 12
- 238000004519 manufacturing process Methods 0.000 claims description 9
- 239000004065 semiconductor Substances 0.000 claims description 9
- 239000000203 mixture Substances 0.000 claims description 4
- 239000013078 crystal Substances 0.000 description 6
- 230000010355 oscillation Effects 0.000 description 6
- 238000005253 cladding Methods 0.000 description 3
- 238000010494 dissociation reaction Methods 0.000 description 2
- 230000005593 dissociations Effects 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000003776 cleavage reaction Methods 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000007791 liquid phase Substances 0.000 description 1
- 239000000155 melt Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- 238000005424 photoluminescence Methods 0.000 description 1
- 230000007017 scission Effects 0.000 description 1
- 238000002791 soaking Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction 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
- H01S5/11—Comprising a photonic bandgap structure
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction 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
- H01S5/12—Construction 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 the resonator having a periodic structure, e.g. in distributed feedback [DFB] lasers
- H01S5/1231—Grating growth or overgrowth details
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Optics & Photonics (AREA)
- Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
- Semiconductor Lasers (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明は、半導体レーザ、特に化合物半導体を
用いた分布帰還型半導体レーザの製造方法に関す
る。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a method for manufacturing a semiconductor laser, particularly a distributed feedback semiconductor laser using a compound semiconductor.
近年、光伝送用光源として従来のフアブリペロ
ー型半導体レーザに代わり、分布帰還型半導体レ
ーザ(以下DFBレーザと略記する)が開発され
ている。DFBレーザを製造するには、周期的な
凹凸構造である回折格子の形成されたInP基板上
にGaInAsPやInP等を多層成長させる必要があ
る。回折格子上にこれらの層を形成するには、従
来600〔℃〕以上の温度で結晶成長を行つている
が、この方法では結晶成長を開始する以前にPの
解離により回折格子が変形するので好ましくな
い。
In recent years, distributed feedback semiconductor lasers (hereinafter abbreviated as DFB lasers) have been developed as light sources for optical transmission in place of conventional Fabry-Perot semiconductor lasers. To manufacture a DFB laser, it is necessary to grow multiple layers of GaInAsP, InP, etc. on an InP substrate on which a diffraction grating, which is a periodic uneven structure, is formed. Conventionally, to form these layers on a diffraction grating, crystal growth is performed at a temperature of 600 [℃] or higher, but with this method, the diffraction grating is deformed due to dissociation of P before crystal growth begins. Undesirable.
そこで最近、600〔℃〕以下の温度で結晶成長を
行う試みが行われている。この方法では、Pの解
離度が著しく減少するので、回折格子を殆んど変
形させることなくその上に結晶成長を行うことが
できる。しかしながら、600〔℃〕以下の成長温度
でバンドギヤツプ波長1.3〔μm〕付近のGaInAsP
活性層を成長しようとすると、GaInAsPのミシ
ビリテイ・ギヤツプの存在領域にかかることがあ
り、結晶性の良い膜を得ることは困難である。こ
のため、DFBレーザの発振しきい値が高くなり
易いと云う問題があつた。 Recently, attempts have been made to grow crystals at temperatures below 600 degrees Celsius. In this method, since the degree of dissociation of P is significantly reduced, crystal growth can be performed on the diffraction grating without substantially deforming it. However, GaInAsP with a bandgap wavelength of around 1.3 [μm] at a growth temperature below 600 [℃]
When attempting to grow an active layer, it may grow in the region where the GaInAsP miscibility gap exists, making it difficult to obtain a film with good crystallinity. For this reason, there has been a problem that the oscillation threshold of the DFB laser tends to become high.
本発明の目的は、回折格子の変形を招くことな
く、結晶性の良い活性層を成長形成することがで
き、DFBレーザの低しきい値発振を可能にする
半導体レーザの製造方法を提供することにある。
An object of the present invention is to provide a method for manufacturing a semiconductor laser that can grow an active layer with good crystallinity without causing deformation of the diffraction grating, and that enables low threshold oscillation of a DFB laser. It is in.
〔発明の概要〕
本発明の骨子は、回折格子の形成された基板上
に低温で光導波路層を成長形成すると共に、この
光導波路層上に高温で活性層を成長形成すること
にある。[Summary of the Invention] The gist of the present invention is to grow an optical waveguide layer at a low temperature on a substrate on which a diffraction grating is formed, and to grow an active layer on the optical waveguide layer at a high temperature.
すなわち本発明は、InP/GaInAsP系半導体レ
ーザを製造する方法において、InP基板上に所定
周期の回折格子を形成したのち、600〔℃〕以下の
温度で上記基板上にGaxIn1-xAsyP1-y光導波路層
を成長形成し、次いで600〔℃〕を越える温度で上
記光導波路層上にGax′In1-x′Asy′P1-y′(x′>x,
y′>y)活性層を成長形成するようにした方法で
ある。 That is, the present invention provides a method for manufacturing an InP/GaInAsP semiconductor laser, in which a diffraction grating with a predetermined period is formed on an InP substrate, and then Ga x In 1-x As is formed on the substrate at a temperature of 600 [°C] or less. y P 1-y optical waveguide layer is grown and then Ga x ′In 1-x ′As y ′P 1-y ′(x′>x,
y′>y) This is a method in which the active layer is grown and formed.
本発明によれば、600〔℃〕以下の温度で回折格
子上に光導波路層を成長形成しているので、この
成長層形成の際に回折格子が変形することはな
い。さらに、600〔℃〕を越える温度で活性層を成
長形成しているので、活性層の結晶性を良好なも
のとすることができる。このため、発振しきい値
を小さくすることができる。また、従来方法に比
し、成長温度を変えるのみで容易に実施し得る等
の利点がある。
According to the present invention, since the optical waveguide layer is grown on the diffraction grating at a temperature of 600 [° C.] or lower, the diffraction grating is not deformed during the formation of this grown layer. Furthermore, since the active layer is grown at a temperature exceeding 600 [° C.], the active layer can have good crystallinity. Therefore, the oscillation threshold can be reduced. Furthermore, compared to conventional methods, this method has the advantage that it can be easily implemented by simply changing the growth temperature.
第1図a〜cは本発明の一実施例に係わる
DFBレーザ製造工程を示す断面図である。まず、
第1図aに示す如くn−InP基板1上に周期2000
〔Å〕,深さ800〔Å〕の回折格子2を形成した。次
いで、第1図bに示す如くn−InP基板1上にn
−Ga0.14In0.86As0.31P0.69層(光導波路層)3を0.2
〔μm〕成長形成した。この光導波路層3の形成に
は液相成長法を用い、第2図に示す如くn−InP
基板1を600〔℃〕でソークしたのち、時刻t1(温
度588℃)から結晶成長を開始した。このとき、
成長温度が600〔℃〕以下であることから、回折格
子2の変形は殆んど生じない。
Figures 1a to 1c relate to an embodiment of the present invention.
FIG. 3 is a cross-sectional view showing a DFB laser manufacturing process. first,
As shown in Figure 1a, the period 2000 is
[Å], and a depth of 800 [Å] was formed. Next, as shown in FIG. 1b, n-InP substrate 1 is
-Ga 0.14 In 0.86 As 0.31 P 0.69 layer (optical waveguide layer) 3 to 0.2
[μm] grew and formed. This optical waveguide layer 3 is formed using a liquid phase growth method, and as shown in FIG.
After soaking the substrate 1 at 600 [°C], crystal growth was started at time t 1 (temperature 588°C). At this time,
Since the growth temperature is 600 [° C.] or lower, almost no deformation of the diffraction grating 2 occurs.
光導波路層3の成長形成後、直ちに基板1を昇
温し670〔℃〕に保つてメルトを均一にしたのち、
時刻t2(温度646℃)から再び結晶成長を開始し
た。すなわち、光導波路層3上に第1図cに示す
如くn−InP層(バツフア層)4、Ga0.26In0.74
As0.56P0.44層(活性層)5、P−InP層(クラツ
ド層)6及びP―Ga0.16In0.84As0.36FP0.64層(キ
ヤツプ層)7を順次連続成長させた。このとき、
活性層5は600〔℃〕を越える温度で成長形成され
るので結晶性の良好なものとなる。また、600
〔℃〕を越える温度であつても、回折格子2上は
前の成長工程により光導波路層3で覆われている
ので、この成長工程で回折格子2が変形する虞れ
はない。 Immediately after the optical waveguide layer 3 was grown and formed, the temperature of the substrate 1 was raised and maintained at 670 [°C] to make the melt uniform.
Crystal growth started again at time t 2 (temperature 646°C). That is, as shown in FIG. 1c, an n-InP layer (buffer layer) 4 and a Ga 0.26 In 0.74
An As 0.56 P 0.44 layer (active layer) 5, a P--InP layer (cladding layer) 6, and a P--Ga 0.16 In 0.84 As 0.36 FP 0.64 layer (cap layer) 7 were successively grown. At this time,
Since the active layer 5 is grown at a temperature exceeding 600[° C.], it has good crystallinity. Also, 600
Even if the temperature exceeds [° C.], the top of the diffraction grating 2 is covered with the optical waveguide layer 3 due to the previous growth process, so there is no risk that the diffraction grating 2 will be deformed during this growth process.
かくして作成されたウエハを評価したところ、
n−InP基板1と光導波路層3との界面には深さ
800〔Å〕の回折格子2が観察された。また、バツ
フア層4は0.1〔μm〕、活性層5は0.2〔μm〕、クラ
ツド層6は2〔μm〕、キヤツプ層7は1〔μm〕で
あり、活性層5のホトルミネツセンス強度は600
〔℃〕以下の温度で成長したものに比べ数倍の強
さであつた。このウエハにストライプ電極を付
け、へき開により素子を作成してその特性を調べ
たところ、約100〔mA〕のしきい値で室温CW・
DFB発振が得られた。これは、全ての層を600
〔℃〕以下の低温で作つた場合に得られるしきい
値200〔mA〕の1/2の値である。 When the wafer thus produced was evaluated,
There is a depth at the interface between the n-InP substrate 1 and the optical waveguide layer 3.
A diffraction grating 2 of 800 [Å] was observed. Further, the buffer layer 4 is 0.1 [μm], the active layer 5 is 0.2 [μm], the cladding layer 6 is 2 [μm], and the cap layer 7 is 1 [μm], and the photoluminescence intensity of the active layer 5 is 600
It was several times stronger than those grown at temperatures below [°C]. Striped electrodes were attached to this wafer, devices were made by cleavage, and their characteristics were investigated.
DFB oscillation was obtained. This will convert all layers to 600
This value is 1/2 of the threshold value of 200 [mA] obtained when manufacturing at a low temperature below [℃].
このように本実施例方法によれば、600〔℃〕以
下の低温(588℃)で光導波路層3を成長形成し、
600〔℃〕を越える温度(646℃)で活性層5を成
長形成しているので、回折格子2の変形を招くこ
となく良質の活性層5を形成することができる。
このため、回折効率及び発光効率が共に向上し、
低しきい値のDFB発振を実現することができる。 As described above, according to the method of this embodiment, the optical waveguide layer 3 is grown and formed at a low temperature of 600 [°C] or lower (588°C),
Since the active layer 5 is grown and formed at a temperature exceeding 600 [°C] (646°C), the active layer 5 of good quality can be formed without causing deformation of the diffraction grating 2.
Therefore, both diffraction efficiency and luminous efficiency are improved,
Low threshold DFB oscillation can be achieved.
なお、本発明は上述した実施例に限定されるも
のではない。例えば、前記光導波路層の成長温度
は588〔℃〕に限定されるものではなく、600〔℃〕
以下の範囲で適宜定めればよい。同様に、活性層
の成長温度は600〔℃〕を越える範囲で適宜定めれ
ばよい。また、活性層及び光導波路層の組成も何
ら実施例に限定されるものではなく、適宜変更可
能である。ただし、本発明が最も有効となるのは
バンドギヤツプ波長λB′が1.20〔μm〕≦λB′≦1.35
〔μm〕であるような発光層(GaInAsP活性層)
を成長させる場合である。したがつて、前記活性
層をなすGax′In1-x′Asy′P1-y′層の組成は(0.20
≦x′≦0.29,0.43≦y′≦0.63)の範囲であるのが
好ましい。さらに、光導波路層のバンドギヤツプ
波長λBはレーザ発振光が吸収を受けないように
1.05〔μm〕≦λB≦1.25〔μm〕の範囲が適当であり、
したがつて前記光導波路層であるGaxIn1-xAsy
P1-y層の組成は(0.10≦x≦0.23,0.21≦y≦
0.50,x<x′,y<y′)の範囲であるのが好まし
い。また、前記基板及び各層の導電型は全て逆に
することも可能である。その他、本発明の要旨を
逸脱しない範囲で、種々変形して実施することが
できる。 Note that the present invention is not limited to the embodiments described above. For example, the growth temperature of the optical waveguide layer is not limited to 588 [°C], but may be 600 [°C].
It may be determined as appropriate within the following range. Similarly, the growth temperature of the active layer may be appropriately set within a range exceeding 600 [°C]. Further, the compositions of the active layer and the optical waveguide layer are not limited to those in the embodiments, and can be changed as appropriate. However, the present invention is most effective when the band gap wavelength λ B ′ is 1.20 [μm]≦λ B ′≦1.35.
[μm] luminescent layer (GaInAsP active layer)
This is the case when growing. Therefore, the composition of the Ga x ′In 1-x ′As y ′P 1-y ′ layer forming the active layer is (0.20
≦x′≦0.29, 0.43≦y′≦0.63). Furthermore, the bandgap wavelength λ B of the optical waveguide layer is set so that the laser oscillation light is not absorbed.
The appropriate range is 1.05 [μm]≦λ B ≦1.25 [μm],
Therefore, the optical waveguide layer Ga x In 1-x As y
The composition of the P 1-y layer is (0.10≦x≦0.23, 0.21≦y≦
0.50, x<x', y<y'). Furthermore, the conductivity types of the substrate and each layer can be reversed. In addition, various modifications can be made without departing from the gist of the present invention.
第1図a〜cは本発明の一実施例に係わる
DFBレーザ製造工程を示す断面図、第2図は上
記実施例工程における処理温度変化を示す模式図
である。
1…n−InP基板、2…回折格子、3…n−
GaInAsP層(光導波路層)、4…n−InP層(バ
ツフア層)、5…GaInAsP層(活性層)、6…P
―InP層(クラツド層)、7…P―GaInAsP層
(キヤツプ層)。
Figures 1a to 1c relate to an embodiment of the present invention.
A cross-sectional view showing the DFB laser manufacturing process, and FIG. 2 are schematic diagrams showing processing temperature changes in the above example process. 1...n-InP substrate, 2...diffraction grating, 3...n-
GaInAsP layer (optical waveguide layer), 4...n-InP layer (buffer layer), 5...GaInAsP layer (active layer), 6...P
-InP layer (cladding layer), 7...P-GaInAsP layer (cap layer).
Claims (1)
工程と、次いで600〔℃〕以下の温度で上記基板上
にGaxIn1-xAsyP1-y光導波路層を成長形成する工
程と、次いで600〔℃〕を越える温度で上記光導波
路層上にGax′In1-x′Asy′P1-y′(x′>x,y′>y
)
活性層を直接若しくはバツフア層を介して成長形
成する工程とを具備したことを特徴とする半導体
レーザの製造方法。 2 前記光導波路層及び活性層の各組成を次のよ
うに設定したことを特徴とする特許請求の範囲第
1項記載の半導体レーザの製造方法。 (0.10≦x≦0.23,0.21≦y≦0.50 0.20≦x′≦0.29,0.43≦y′≦0.63)[Claims] 1. A step of forming a diffraction grating with a predetermined period on an InP substrate, and then forming a Ga x In 1-x As y P 1-y optical waveguide layer on the substrate at a temperature of 600 [°C] or less. Ga x ′In 1-x ′As y ′P 1-y ′ (x′>x, y′>y
)
1. A method for manufacturing a semiconductor laser, comprising the step of growing an active layer directly or via a buffer layer. 2. The method of manufacturing a semiconductor laser according to claim 1, wherein the compositions of the optical waveguide layer and the active layer are set as follows. (0.10≦x≦0.23, 0.21≦y≦0.50 0.20≦x′≦0.29, 0.43≦y′≦0.63)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58085886A JPS59213190A (en) | 1983-05-18 | 1983-05-18 | Manufacture of semiconductor laser |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58085886A JPS59213190A (en) | 1983-05-18 | 1983-05-18 | Manufacture of semiconductor laser |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59213190A JPS59213190A (en) | 1984-12-03 |
| JPS6354236B2 true JPS6354236B2 (en) | 1988-10-27 |
Family
ID=13871387
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58085886A Granted JPS59213190A (en) | 1983-05-18 | 1983-05-18 | Manufacture of semiconductor laser |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59213190A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60206132A (en) * | 1984-03-30 | 1985-10-17 | Nec Corp | Crystal growing process |
| JPH0567848A (en) * | 1991-09-05 | 1993-03-19 | Fujitsu Ltd | Method for manufacturing optical semiconductor device |
-
1983
- 1983-05-18 JP JP58085886A patent/JPS59213190A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59213190A (en) | 1984-12-03 |
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