JPS63142886A - Semiconductor laser device - Google Patents
Semiconductor laser deviceInfo
- Publication number
- JPS63142886A JPS63142886A JP29105386A JP29105386A JPS63142886A JP S63142886 A JPS63142886 A JP S63142886A JP 29105386 A JP29105386 A JP 29105386A JP 29105386 A JP29105386 A JP 29105386A JP S63142886 A JPS63142886 A JP S63142886A
- Authority
- JP
- Japan
- Prior art keywords
- end surfaces
- onto
- active layer
- substrate
- vicinity
- 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
- 239000004065 semiconductor Substances 0.000 title claims description 13
- 239000000758 substrate Substances 0.000 claims abstract description 13
- 230000003287 optical effect Effects 0.000 abstract description 9
- 238000005530 etching Methods 0.000 abstract description 4
- 238000000034 method Methods 0.000 abstract description 4
- 239000007791 liquid phase Substances 0.000 abstract description 3
- 230000000903 blocking effect Effects 0.000 abstract description 2
- 229910001218 Gallium arsenide Inorganic materials 0.000 abstract 1
- 230000015556 catabolic process Effects 0.000 abstract 1
- 238000007493 shaping process Methods 0.000 abstract 1
- 230000000694 effects Effects 0.000 description 6
- 239000013078 crystal Substances 0.000 description 2
- 230000006378 damage Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000003795 chemical substances by application Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】 産業上の利用分野 本発明は、半導体レーザ装置に関するものである。[Detailed description of the invention] Industrial applications The present invention relates to a semiconductor laser device.
従来の技術
半導体レーザ装置は、光デイスク上の信号の読み取りや
レーザビームプリンタの光源、そして光通信にと広く実
用されるに至っている。これらの光情報機器においては
、必要なレーザ出力は20mW以下がほとんどであった
。しかし、近年、光ディスクの書き込みなどの用途に高
出力半導体レーザの要望が益々高まっている。BACKGROUND OF THE INVENTION Semiconductor laser devices have come into widespread use for reading signals on optical disks, as light sources for laser beam printers, and for optical communications. In most of these optical information devices, the required laser output was 20 mW or less. However, in recent years, there has been an increasing demand for high-power semiconductor lasers for applications such as writing on optical discs.
発明が解決しようとする問題点
しかしながら、従来の半導体レーザでは高出力で駆動さ
せると端面の結晶がレーザ光を吸収して溶融する、いわ
ゆる端面破壊を生じるために、安定な高出力動作は困難
とされていた。Problems to be Solved by the Invention However, when conventional semiconductor lasers are driven at high power, the crystals at the end face absorb the laser beam and melt, resulting in so-called end face destruction, making stable high power operation difficult. It had been.
本発明は、前記問題点に鑑み端面破壊を防ぎ、安定な高
出力動作をすることのできる半導体レーザ装置を提供す
るものである。In view of the above-mentioned problems, the present invention provides a semiconductor laser device that can prevent end face breakage and perform stable high output operation.
問題点を解決するための手段
前記問題点を解決するために本発明の半導体レーザ装置
は、基板上に端面近傍での高さが高くなるように2本の
平行なリッジが記載され、前記基板上に活性層を含む各
層が記載されて構成されている。Means for Solving the Problems In order to solve the above-mentioned problems, the semiconductor laser device of the present invention has two parallel ridges written on the substrate so that the height near the end face is high, and Each layer including the active layer is described and configured thereon.
作用
この構成によって、端面近傍での活性層の厚さが薄くな
り、したがって端面でのレーザのスポットサイズが広が
り、光出力密度が下がるために高出力動作が可能となる
。Effect: This configuration reduces the thickness of the active layer in the vicinity of the end facets, thus increasing the laser spot size at the end facets and lowering the optical output density, thereby enabling high power operation.
実施例
以下本発明の第1の実施例について図面を参照しながら
説明する。EXAMPLE A first example of the present invention will be described below with reference to the drawings.
pWGaAs基板1(1oo)面上に(011)方向に
第4図に示すような高さ6μmのメサをエツチングによ
シ形成する。この基板上にn型ブロッキング層2の成長
を行ない、その後成長表面に第1図に示すような2本の
平行なりッジ7をエツチングにより形成する。リッジの
幅は各20μm。A mesa having a height of 6 μm as shown in FIG. 4 is formed in the (011) direction on the pWGaAs substrate 1 (1oo) plane by etching. An n-type blocking layer 2 is grown on this substrate, and then two parallel ridges 7 as shown in FIG. 1 are formed on the growth surface by etching. The width of each ridge is 20 μm.
リッジ間の溝の幅は6μmとする。そして端面より20
μm以内の端面近傍では基板を深くエツチングしてリッ
ジの高さを6μmとし、端面近傍以外のレーザ中央部で
は高さを1.6μmとする。リッジを形成したウェハー
上に液相エピタキシャル法により活性層を含む各層を形
成する。成長を行なったウェハーの表裏にそれぞれオー
ミック電極を形成し、キャビティ長260μmにへき関
し、レーザチップを得る。The width of the groove between the ridges is 6 μm. And from the end face 20
The substrate is deeply etched to have a ridge height of 6 μm near the end face within μm, and the height of the ridge is 1.6 μm at the center of the laser other than near the end face. Each layer including the active layer is formed on the wafer with the ridge formed thereon by a liquid phase epitaxial method. Ohmic electrodes are formed on the front and back surfaces of the grown wafer, and a laser chip is obtained by forming a cavity with a cavity length of 260 μm.
上記の工程で作製したレーザの端面近傍での断面図を第
6図に、レーザ内部での断面図を第6図に示す。FIG. 6 shows a cross-sectional view near the end face of the laser manufactured through the above process, and FIG. 6 shows a cross-sectional view inside the laser.
本実施例の半導体レーザ装置は以上の構成を有するので
以下に述べるような効果がある。Since the semiconductor laser device of this embodiment has the above configuration, it has the following effects.
リッジを有する基板上に液相エピタキシャル法により成
長を行なうと、結晶成長の異方性により、リッジ上での
膜厚は薄くなる。この効果はりッジの高さが高いほど大
きい。そのため、本実施例のように端面近傍でのみ高さ
の高いリッジ上に成長を行なうとレーザ内部に比べて端
面近傍ではより薄い活性層を形成することができる(d
、(d2)。When a film is grown by liquid phase epitaxial method on a substrate having a ridge, the film thickness on the ridge becomes thinner due to the anisotropy of crystal growth. This effect is greater as the height of the ridge is higher. Therefore, if growth is performed on the high ridge only near the end face as in this example, a thinner active layer can be formed near the end face than inside the laser (d
, (d2).
この結果、端面近傍では活性層4からクラブト層(3お
よび5)へ光が大きく広がるためにレーザのスポットサ
イズが広がり、光出力密度が下がる。As a result, in the vicinity of the end face, light widely spreads from the active layer 4 to the Crabstone layers (3 and 5), so the spot size of the laser increases and the optical output density decreases.
そのため、端面破壊を生じる最大光出力が上昇し、より
高出力での動作が可能となる。Therefore, the maximum optical output that causes end face destruction increases, making it possible to operate at higher output.
第2図は第2の実施例の端面近傍での断面図を示す。第
6図と比較すればわかるように、第2の実施例ではりッ
ジ7の間の溝の深さは一定で、リッジの外側のみ端面近
傍で深くなっている構造であるが、第1の実施例と同様
の効果が期待できる。FIG. 2 shows a sectional view near the end face of the second embodiment. As can be seen from a comparison with FIG. 6, in the second embodiment, the depth of the groove between the ridges 7 is constant, and only the outer side of the ridge becomes deeper near the end face. The same effects as in the embodiment can be expected.
第3図は第3の実施例の端面近傍での断面図を示す。第
3の実施例ではn型GaムS基板9を用い、活性層上部
に形成したZn拡散領域8より電流注入を行なう構造と
なっているが、明らかに第1の実施例と同様の効果が期
待できる。FIG. 3 shows a sectional view near the end face of the third embodiment. The third embodiment uses an n-type GaM S substrate 9 and has a structure in which current is injected from the Zn diffusion region 8 formed on the top of the active layer, but it is clear that the same effect as in the first embodiment is obtained. You can expect it.
発明の効果
以上のように本発明は、端面近傍の高さが高くなるよう
に2つの平行なりッジが記載された基板の上に、活性層
を含む各層が記載されることにより、端面でのスポット
サイズが広がり、高出方動作が可能となる。Effects of the Invention As described above, the present invention provides a structure in which each layer including the active layer is written on a substrate on which two parallel ridges are written so that the height near the end face is high. The spot size is expanded and high output operation is possible.
第1図は本発明の半導体レーザ装置の第1の実施例の構
造図、第2図は本発明の半導体レーザ装置の第2の実施
例の端面近傍での構造断面図、第3図は本発明の半導体
レーザ装置の第3の実施例の端面近傍での構造断面図、
第4図は本発明の半導体レーザ装置の第1の実施例の作
製工程の途中を示す図、第6図は本発明の第1の実施例
の端面近傍断面図、第6図は本発明の第1の実施例のレ
ーザ内部断面図である。
1・・・・・・p型GaAS基板、2・・・・・・n型
GaAS層、3・・・・・・pWGaA5As層、4・
・・・・・G&ムlムS活性層。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名t−
−−p竺hh基試FIG. 1 is a structural diagram of a first embodiment of the semiconductor laser device of the present invention, FIG. 2 is a structural cross-sectional view near the end face of the second embodiment of the semiconductor laser device of the present invention, and FIG. A structural sectional view near the end face of a third embodiment of the semiconductor laser device of the invention,
FIG. 4 is a diagram showing the middle of the manufacturing process of the first embodiment of the semiconductor laser device of the present invention, FIG. 6 is a sectional view near the end face of the first embodiment of the present invention, and FIG. FIG. 3 is an internal cross-sectional view of the laser of the first embodiment. 1... p-type GaAS substrate, 2... n-type GaAS layer, 3... pWGaA5As layer, 4...
...G & Murmu S active layer. Name of agent: Patent attorney Toshio Nakao and one other person
--pjihh base test
Claims (1)
おけるよりも高く形成された基板上に、活性層を含む複
数の層が形成されている半導体レーザ装置。A semiconductor laser device in which a plurality of layers including an active layer are formed on a substrate in which two parallel ridges are formed higher near the laser end face than in the center.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29105386A JPS63142886A (en) | 1986-12-05 | 1986-12-05 | Semiconductor laser device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29105386A JPS63142886A (en) | 1986-12-05 | 1986-12-05 | Semiconductor laser device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63142886A true JPS63142886A (en) | 1988-06-15 |
Family
ID=17763819
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP29105386A Pending JPS63142886A (en) | 1986-12-05 | 1986-12-05 | Semiconductor laser device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63142886A (en) |
-
1986
- 1986-12-05 JP JP29105386A patent/JPS63142886A/en active Pending
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