JPH03187283A - Method of forming active region - Google Patents
Method of forming active regionInfo
- Publication number
- JPH03187283A JPH03187283A JP32624189A JP32624189A JPH03187283A JP H03187283 A JPH03187283 A JP H03187283A JP 32624189 A JP32624189 A JP 32624189A JP 32624189 A JP32624189 A JP 32624189A JP H03187283 A JPH03187283 A JP H03187283A
- Authority
- JP
- Japan
- Prior art keywords
- crystal growth
- diffusion
- active layer
- drive
- active region
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 238000000034 method Methods 0.000 title claims description 13
- 238000009792 diffusion process Methods 0.000 claims abstract description 27
- 239000013078 crystal Substances 0.000 claims abstract description 19
- 239000004065 semiconductor Substances 0.000 claims abstract description 12
- 238000004519 manufacturing process Methods 0.000 claims description 3
- 230000002349 favourable effect Effects 0.000 abstract 1
- 238000005253 cladding Methods 0.000 description 11
- 239000000758 substrate Substances 0.000 description 4
- 230000000903 blocking effect Effects 0.000 description 3
- 238000007796 conventional method Methods 0.000 description 3
- 229910052581 Si3N4 Inorganic materials 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 230000002265 prevention Effects 0.000 description 2
- 239000010409 thin film Substances 0.000 description 2
- 238000007740 vapor deposition Methods 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、拡散によって活性部を形成する半導体レー
ザの製作法に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a method for manufacturing a semiconductor laser in which an active region is formed by diffusion.
第3図及び第4図は従来の半導体レーザの活性領域形成
方法の工程を示す半導体レーザの断面図である。図にお
いて、(1)は、第1の導電型の半導体基板、(2)は
第1の導電型のクラッド層、(3)は第1の導電型の活
性層、(4)は第1の導電型のクラッド層、(5)は第
2の導電型の電流阻止層、(6)は第1の導電型のコン
タクト層、(7)は拡散源の例えばSi3N4のマスク
、(8)は例えばZnOの第2の導電型の拡散源、(9
)は拡散源(8)の空中への飛散を防ぐ例えば5in2
のカバー、00は拡散源、(8)が拡散した拡散領域、
Ol)はドライブのための例えばSi、N4のカバー叫
は拡散およびドライブfこよって形成されたドライブ領
域である。3 and 4 are cross-sectional views of a semiconductor laser showing the steps of a conventional method for forming an active region of a semiconductor laser. In the figure, (1) is a semiconductor substrate of a first conductivity type, (2) is a cladding layer of a first conductivity type, (3) is an active layer of a first conductivity type, and (4) is a semiconductor substrate of a first conductivity type. A cladding layer of a conductive type, (5) a current blocking layer of a second conductive type, (6) a contact layer of a first conductive type, (7) a mask of a diffusion source such as Si3N4, and (8) a mask of, for example, Si3N4. a diffusion source of the second conductivity type of ZnO, (9
) is for example 5in2 to prevent the diffusion source (8) from scattering into the air.
, 00 is the diffusion source, (8) is the diffused area,
OL) is a cover of Si, N4, for example, for the drive, and is the drive region formed by the diffusion and drive f.
次に形成方法について説明する。先ず第3図に示すごと
く半導体基板(1)上にクラッド層(2)、活性m (
31、クラッド層(4)、電流阻止層(5)、コンタク
ト層(6)を順次結晶成長したウニハモに、マスク(7
)を形成し、拡散源(8)およびカバー(9)を蒸着形
成する。Next, the formation method will be explained. First, as shown in FIG. 3, a cladding layer (2) and an active layer m (
31. A mask (7
), and a diffusion source (8) and a cover (9) are formed by vapor deposition.
次いで、約600〜700℃に全体を熱することにより
、拡散源(8)が、マスク(7)の無い場所のみからコ
ンタクト層(6111E流阻止層(5)、クラッドm(
4)へと拡散する。次に第4図に示すごとくカバー(9
)、拡散源(8)、マスク(7)を取り除き、カバーθ
υを全面に蒸着形成する。そして全体を900〜950
℃でドライブし、拡散領域(lαより更に拡げ、ドライ
ブによって形成されたドライブ領域02)を製作する。Next, by heating the whole to about 600-700°C, the diffusion source (8) spreads the contact layer (6111E flow prevention layer (5), cladding m (
4). Next, as shown in Figure 4, the cover (9
), remove the diffusion source (8) and mask (7), and cover θ
υ is deposited on the entire surface. And the whole 900-950
℃ to produce a diffusion region (drive region 02 further expanded from lα and formed by the drive).
このドライブ領域a目よ、第1の導電型の活性層(3)
に達するため、この部分のみが第2の導電型に変化、活
性領域を形成することができる。This drive region a, first conductivity type active layer (3)
Therefore, only this portion can change to the second conductivity type and form an active region.
従来の活性領域形成方法は以とのように行なわれている
ので、クラッド層および電流阻止層は、活性層の光を減
衰させないために1例えば11tm程度以下に薄くする
ことはできず、そのためドライブ領域が活性層進達する
ように拡散およびドライブすると、ドライブ領域が横方
向にも例えば2〜3p、m程度に拡がって、狭くするこ
とが難かしく、また、ドライブ領域が少しずれたtごけ
で活性領域の幅が大きく変化し、制御性が悪いなどの問
題点があった。The conventional active region forming method is carried out as follows, so the cladding layer and the current blocking layer cannot be made thinner than 1, for example, 11 tm, in order not to attenuate the light in the active layer. If the region is diffused and driven so as to advance into the active layer, the drive region will spread laterally to about 2 to 3 meters, making it difficult to narrow it. There were problems such as the width of the active region changed significantly and controllability was poor.
この発明は上記のような問題点を解消するためになされ
たもので、ドライブ領域の幅を狭く、シかも制御性よく
形成できる方法を得ることを目的とする。The present invention was made to solve the above-mentioned problems, and it is an object of the present invention to provide a method by which the width of the drive area can be narrowed and the width can be formed with good controllability.
この発明に係る活性領域形成方法は、活性層上に薄膜を
成長させた時点で1回目の結晶成長を止め、拡散は従来
の方法を用い、特別なドライブの工程を経ずに2回目の
結晶成長を行なうものである。In the active region forming method according to the present invention, the first crystal growth is stopped when a thin film is grown on the active layer, the diffusion is performed using a conventional method, and the second crystal growth is performed without going through a special drive process. It is about growth.
この発明における2回目の結晶成長は、結晶成長と同時
にドライブも自然に行なわれ、活性領域を形成する。In the second crystal growth in this invention, driving is performed naturally at the same time as the crystal growth, and an active region is formed.
以下、この発明の一実施例を図について説明する。第1
図及び第2図は活性領域形成方法の工程を示す半導体レ
ーザの断面図である。図において(1)から02)まで
は第3図及び第4図の従来例に示したものと同等である
ので説明を省略する。(4a)は、1回目の結晶成長で
形成した第1導電型のクラッド層、 (4b)は2回
目の結晶成長で形成した第1導電型のクラッド層である
。An embodiment of the present invention will be described below with reference to the drawings. 1st
1 and 2 are cross-sectional views of a semiconductor laser showing steps of an active region forming method. In the figure, the steps (1) to 02) are the same as those shown in the conventional example of FIGS. 3 and 4, and therefore their explanation will be omitted. (4a) is a cladding layer of the first conductivity type formed in the first crystal growth, and (4b) is a cladding layer of the first conductivity type formed in the second crystal growth.
次に活性領域の形成方法について説明する。まず、第1
図のごとく、半導体基板(1)の丘に、クラッド層(2
)、活性層(3)、クラッド層(4a)を順次結晶成長
させ、そのLにマスク(7)を形成し、拡散源(8)お
よびカバー(9)を蒸着形成する。次いで約600〜7
00℃に全体を熱することにより、拡散源(8)がマス
ク(7)の無い場所のみから、クラッド層(4a)へと
拡散する。次に第2図に示すごとくカバー(9)。Next, a method for forming the active region will be explained. First, the first
As shown in the figure, the cladding layer (2) is placed on the hill of the semiconductor substrate (1).
), an active layer (3), and a cladding layer (4a) are successively crystal-grown, a mask (7) is formed on the L, and a diffusion source (8) and a cover (9) are formed by vapor deposition. Then about 600-7
By heating the whole to 00° C., the diffusion source (8) diffuses into the cladding layer (4a) only from the area where there is no mask (7). Next, as shown in Figure 2, cover (9).
拡散源(8)、マスク(7)を取り除き、そのLにクラ
ラ)’11 (4b) 、 [流阻止/1(51,:1
ンタクト層(6)を結晶成長する。この結晶成長する際
の温度は例えば750〜850℃で、結晶成品している
間に拡散領域(101が自然にドライブされ、ドライブ
領域02)を形成する。このドライブ領域02:Jは、
活性層(3)に達するため、この部分のみが第2導電型
に変化し、活性領域0○を形成することができる。この
ように、わずかな領域のみを拡散ドライブすれば良いの
で。Remove the diffusion source (8) and the mask (7), and put Clara on its L)'11 (4b), [Flow prevention/1 (51,:1
A contact layer (6) is crystal grown. The temperature during this crystal growth is, for example, 750 to 850° C., and a diffusion region (101 is naturally driven to form a drive region 02) while the crystal is being formed. This drive area 02:J is
Since it reaches the active layer (3), only this portion changes to the second conductivity type, and an active region 0○ can be formed. In this way, you only need to drive the diffusion in a small area.
幅の狭い活性領域が実現でき、横モードを安定にするこ
とができる。また、拡散領域001. ドライブ領域
02)が小さいので、制御性も良くなる。A narrow active region can be realized, and the transverse mode can be stabilized. In addition, the diffusion region 001. Since the drive area 02) is small, controllability is also improved.
以上のように、この発明によれば、活性層上に薄膜を成
長させた時点で1回目の成長を止め、拡散は従来の方法
を用いるが、2回目の結晶成長時にドライブを同時に行
なうので、狭い活性領域が実現でき、制御性も向上する
効果がある。As described above, according to the present invention, the first growth is stopped when a thin film is grown on the active layer, and the conventional method is used for diffusion, but the driving is performed simultaneously during the second crystal growth. This has the effect of realizing a narrow active region and improving controllability.
【図面の簡単な説明】
第1図及び第2図はこの発明の一実施例による活性領域
形成方法の工程を示す半導体レーザの断面図、第3図及
び第4図は従来の活性領域形成方法の工程を示す半導体
レーザの断面図である。図において(1)は半導体基板
、 f21 、 (4) 、 (4a)、(4b)はク
ラッド層、(3)は活性層、(5)は電流阻止層、(6
)はコンタクト層、(7)はマスク、(8)は拡散源、
(9)。
(II)はカバー、 (101は拡散領域、a幻はドラ
イブ領域である。
なお、図中、同一符号は同一、又は相当部分を示す。[BRIEF DESCRIPTION OF THE DRAWINGS] FIGS. 1 and 2 are cross-sectional views of a semiconductor laser showing steps of an active region forming method according to an embodiment of the present invention, and FIGS. 3 and 4 are sectional views of a conventional active region forming method. FIG. 3 is a cross-sectional view of a semiconductor laser showing the process of FIG. In the figure, (1) is a semiconductor substrate, f21, (4), (4a), (4b) are cladding layers, (3) is an active layer, (5) is a current blocking layer, (6)
) is the contact layer, (7) is the mask, (8) is the diffusion source,
(9). (II) is a cover, (101 is a diffusion area, and phantom a is a drive area. In the figures, the same reference numerals indicate the same or corresponding parts.
Claims (1)
結晶成長を活性層上部0.5μm以下の厚さで止め、次
いで活性層に達しない程度に選択拡散を行ない、次に2
回目の結晶成長を行ない、成長と同時に熱により拡散源
を活性層まで選択的に到達させて活性部を製作すること
を特徴とする活性領域形成方法。In the semiconductor laser manufacturing process that includes diffusion, the first crystal growth is stopped at a thickness of 0.5 μm or less above the active layer, then selective diffusion is performed to the extent that it does not reach the active layer, and then the second crystal growth is performed.
A method for forming an active region, characterized in that an active region is produced by performing a second crystal growth, and simultaneously causing a diffusion source to selectively reach the active layer using heat at the same time as the crystal growth.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP32624189A JPH03187283A (en) | 1989-12-16 | 1989-12-16 | Method of forming active region |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP32624189A JPH03187283A (en) | 1989-12-16 | 1989-12-16 | Method of forming active region |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03187283A true JPH03187283A (en) | 1991-08-15 |
Family
ID=18185573
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP32624189A Pending JPH03187283A (en) | 1989-12-16 | 1989-12-16 | Method of forming active region |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03187283A (en) |
-
1989
- 1989-12-16 JP JP32624189A patent/JPH03187283A/en active Pending
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