JPH077848B2 - Edge emitting type light emitting diode - Google Patents
Edge emitting type light emitting diodeInfo
- Publication number
- JPH077848B2 JPH077848B2 JP9220787A JP9220787A JPH077848B2 JP H077848 B2 JPH077848 B2 JP H077848B2 JP 9220787 A JP9220787 A JP 9220787A JP 9220787 A JP9220787 A JP 9220787A JP H077848 B2 JPH077848 B2 JP H077848B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- light emitting
- led
- type
- groove
- 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 - Lifetime
Links
- 239000000758 substrate Substances 0.000 claims description 10
- 238000002347 injection Methods 0.000 claims description 5
- 239000007924 injection Substances 0.000 claims description 5
- 230000000903 blocking effect Effects 0.000 claims description 4
- 239000004065 semiconductor Substances 0.000 claims description 2
- 230000010355 oscillation Effects 0.000 description 9
- 230000007547 defect Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 5
- 238000004519 manufacturing process Methods 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000005253 cladding Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000002950 deficient Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000013307 optical fiber Substances 0.000 description 1
- 229920002120 photoresistant polymer Polymers 0.000 description 1
Landscapes
- Led Devices (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は端面発光型発光ダイオードの構造に関する。The present invention relates to a structure of an edge emitting light emitting diode.
端面発光型発光ダイオード(LED)は光ファイバーとの
カップリング効率が高いという特徴を有しているために
通信用の光源として有望視されている。従来、この種の
LEDとして結晶内部に電流ブロック層を設けたLEDが知ら
れているが、これは第2図に示すようにp型InP基板1
上に該基板と反対の導電型を有するn型InP電流ブロッ
ク層2を形成したのち、少なくとも基板1に達する深さ
の一定の幅の溝7を設け、しかるのち溝内及び溝外上に
基板1と同じ導電型のp型InPクラッド層3、p型InGaA
sP活性層4、n型InPクラッド層5及びn型InGaAsPキャ
ップ層6を形成した構造を有していた。従って、基板よ
り注入された電流は溝部を経て、活性層へと注入されて
ゆくが、素子長全域で溝幅が同じ幅であるため、活性層
へ注入される電流の電流密度は素子長方向では差はなか
った。The edge emitting type light emitting diode (LED) is regarded as a promising light source for communication because it has a feature of high coupling efficiency with an optical fiber. Traditionally, this kind of
As an LED, an LED in which a current block layer is provided inside a crystal is known. This is a p-type InP substrate 1 as shown in FIG.
After forming an n-type InP current blocking layer 2 having a conductivity type opposite to that of the substrate, a groove 7 having a constant width with a depth reaching at least the substrate 1 is provided, and thereafter, the substrate is provided inside and outside the groove. P-type InP clad layer 3 of the same conductivity type as 1 and p-type InGaA
The sP active layer 4, the n-type InP clad layer 5, and the n-type InGaAsP cap layer 6 were formed. Therefore, the current injected from the substrate is injected into the active layer through the groove. However, since the groove width is the same across the entire element length, the current density of the current injected into the active layer is in the element length direction. So there was no difference.
上述した従来の端面発光LEDは、電流狭窄のための溝構
造が発光面から反射面までの全面に施してあるので注入
電流が高くなると、素子端面のへき開面が共振器となっ
てレーザ発振を起こししきい値が発生するために、電流
−光出力特性の線形成が失われる。さらに温度による電
流光出力特性曲線の変化が著るしくなるため、LED用の
駆動用回路では、出力の制御が困難になるという欠点が
あった。In the above-mentioned conventional edge emitting LED, the groove structure for current confinement is provided on the entire surface from the light emitting surface to the reflecting surface, so when the injected current becomes high, the cleaved surface of the element end surface becomes a resonator to cause laser oscillation. Due to the raising threshold, the line formation of the current-light output characteristic is lost. Furthermore, since the current-light output characteristic curve changes significantly with temperature, the LED driving circuit has a drawback that it is difficult to control the output.
本発明は、電流狭窄のための溝部の溝幅を発光面から反
射面ヘ向けて連続的に狭めることにより素子内で電流注
入密度を変化させ、発光面側では利得が大きく反射面側
では損失が大きくなる構造とすることにより、高電流密
度に対しても良好なLED特性を示す端面発光型LEDを提供
するものである。The present invention changes the current injection density in the element by continuously narrowing the groove width of the groove portion for current constriction from the light emitting surface to the reflecting surface, resulting in a large gain on the light emitting surface side and a loss on the reflecting surface side. By providing a structure having a large LED, an edge emitting LED that exhibits excellent LED characteristics even at high current densities is provided.
次に本発明についてInP-InGaAsPを半導体層として用い
た場合の実施例を図面を参照して説明する。第1図
(A),(B),(C)は本発明の第1の実施例の素子
の各主要部の製造工程を示す斜視図である。まず、第1
図(A)に示すようにp型InP基板1上にn型InP電流ブ
ロック層2を成長させる。次いで第1図(B)に示すよ
うにn型InPブロック層2上にフォトレジスト膜をマス
クとして選択エッチングで発光側面での溝幅9μm、反
射側面での溝幅0の同じ深さの溝8を形成する。その上
に第1図(C)に示すように、p型Inクラッド層3、p
型InGaAsP活性層4、n型InPクラッド層5、およびn型
InGaAsPキャップ層6を連続成長する。そして両面に電
極を設けてLEDは完成する。素子長は約300μmである。Next, the present invention will be described with reference to the drawings with respect to an embodiment in which InP-InGaAsP is used as a semiconductor layer. FIGS. 1 (A), (B), and (C) are perspective views showing the manufacturing process of each main part of the device of the first embodiment of the present invention. First, the first
An n-type InP current blocking layer 2 is grown on a p-type InP substrate 1 as shown in FIG. Then, as shown in FIG. 1B, a groove 8 of the same depth having a groove width of 9 μm on the light emitting side surface and a groove width of 0 on the reflective side surface is selectively etched by using the photoresist film as a mask on the n-type InP block layer 2. To form. On top of that, as shown in FIG. 1 (C), the p-type In cladding layer 3, p
-Type InGaAsP active layer 4, n-type InP clad layer 5, and n-type
The InGaAsP cap layer 6 is continuously grown. The LED is completed by providing electrodes on both sides. The element length is about 300 μm.
このようにして製作したLEDの電極に電圧を印加して電
流を流すと、電流はp型InP基板1より溝8中を通って
p型InPクラッド層3、p型InGaAsP活性層4、n型InP
クラッド層5、n型InGaAsPキャップ層6へと流れる。
ここで活性層4へ注入される電流密度は、p型InPクラ
ッド層3での電流横広がりのため、溝中での電流密度よ
りも小さく、かつ溝幅が発光面側から反射面側へ向け
て、徐々に狭くなっているため反射面側付近の領域では
活性層への注入電流密度は発光面側付近の領域に比べか
なり小さくなっている。この結果反射面側付近の領域で
は、レーザー発振を起こす利得には達しにくく、逆にレ
ーザー発振を妨げる効果をもたらす。When a voltage is applied to the electrode of the LED thus manufactured and a current is caused to flow, the current passes through the groove 8 from the p-type InP substrate 1, the p-type InP clad layer 3, the p-type InGaAsP active layer 4, and the n-type. InP
It flows to the clad layer 5 and the n-type InGaAsP cap layer 6.
The current density injected into the active layer 4 is smaller than the current density in the groove due to the lateral spread of the current in the p-type InP clad layer 3, and the groove width is directed from the light emitting surface side to the reflective surface side. Since it is gradually narrowed, the current density injected into the active layer in the region near the reflecting surface side is considerably smaller than that in the region near the light emitting surface side. As a result, in the region near the reflecting surface side, it is difficult to reach the gain that causes laser oscillation, and on the contrary, the effect of hindering laser oscillation is brought about.
次に、具体的効果をデータをもとにして説明する。第3
図は、本発明の端面発光型LEDの電流−光出力特性の実
験結果である。破線で示す従来例では約20mAの注入電流
でレーザー発振を起こし、20mA以上の注入電流に対して
はLED特性を得ることができなかった。これに対し実線
で示す本発明による端面発光型LEDにおいてはレーザー
発振をおこさず、80mAまで良好なLED特性を示した。Next, specific effects will be described based on data. Third
The figure shows the experimental results of the current-light output characteristics of the edge emitting LED of the present invention. In the conventional example shown by the broken line, laser oscillation occurred with an injection current of about 20 mA, and the LED characteristics could not be obtained for an injection current of 20 mA or more. On the other hand, the edge emitting LED according to the present invention shown by the solid line did not cause laser oscillation and showed good LED characteristics up to 80 mA.
次に本発明の第2の実施例として、n型InP電流ブロッ
ク層2の上に発光面での溝幅9μm、反射面での溝幅3
μmの溝を形成したLEDを製作した。Next, as a second embodiment of the present invention, a groove width of 9 μm on the light emitting surface and a groove width of 3 on the reflecting surface are formed on the n-type InP current blocking layer 2.
An LED with a groove of μm was manufactured.
第4図は30mAの注入電流に対するレーザー発振による不
良率を調査した結果を示すグラフである。縦軸にレーザ
ー発振による不良率、横軸は発光面における溝幅に対す
る反射面の溝幅の割合いを示す。従来のLEDは、横軸1
の場合であり、不良率50%であった。本発明による第2
の実施例のLEDは横軸3/9の場合で、その不良率は12%で
あり、第1の実施例のLEDは横軸0の場合で、その不良
率は5%であった。第2の実施例において、電流−光出
力特性を調べたところ、第1の実施例と同様の効果を得
た。FIG. 4 is a graph showing the results of investigating the defect rate due to laser oscillation with respect to an injection current of 30 mA. The vertical axis represents the defect rate due to laser oscillation, and the horizontal axis represents the ratio of the groove width of the reflecting surface to the groove width of the light emitting surface. Conventional LED has 1 horizontal axis
And the defective rate was 50%. Second according to the present invention
The LED of Example 1 had a defect rate of 12% when the horizontal axis was 3/9, and the LED of the first example had a defect rate of 5% when the horizontal axis was 0. When the current-light output characteristics were examined in the second example, the same effect as in the first example was obtained.
以上説明したように、本発明は、端面発光型LEDにおい
て素子内に溝幅が連続的に変化する電流狭窄構造を有す
ることにより、素子内の電流密度に変化をもたせてレー
ザー発振を防止し、高出力の良好なLEDを高歩留りで得
ることができる効果がある。As described above, the present invention prevents the laser oscillation by changing the current density in the element by having the current confinement structure in which the groove width is continuously changed in the element in the edge emitting LED. There is an effect that a good LED with high output can be obtained with high yield.
第1図(A)〜(C)は本発明の第1の実施例における
端面発光型LEDの製造工程を示す斜視図、第2図(A)
〜(C)は従来の端面発光型LEDの製造工程を示す斜視
図、第3図は本発明の端面発光型LEDの電流−光出力特
性を示す図、第4図は本発明の端面発光型LEDのレーザ
ー発振による不良率と従来の場合の比較図である。 1……p型InP基板、2……n型InPブロック層、3……
p型InPクラッド層、4……p型InGaAsP活性層、5……
n型InPクラッド層、6……n型InGaAsPキャップ層、7,
8……溝。1 (A) to 1 (C) are perspective views showing a manufacturing process of an edge emitting LED according to the first embodiment of the present invention, and FIG. 2 (A).
(C) is a perspective view showing a manufacturing process of a conventional edge emitting LED, FIG. 3 is a diagram showing current-light output characteristics of the edge emitting LED of the present invention, and FIG. 4 is an edge emitting type of the present invention. FIG. 8 is a comparison diagram of a defect rate due to laser oscillation of an LED and a conventional case. 1 ... p-type InP substrate, 2 ... n-type InP block layer, 3 ...
p-type InP clad layer, 4 ... p-type InGaAsP active layer, 5 ...
n-type InP clad layer, 6 ... n-type InGaAsP cap layer, 7,
8 …… Groove.
Claims (1)
に基板に達するストライプ状の溝を形成して注入電流を
狭窄する端面発光型発光ダイオードにおいて、前記溝の
溝幅を発光面側から反射面側へ連続的に狭めて電流注入
領域を制限したことを特徴とする端面発光型発光ダイオ
ード。1. An edge emitting light emitting diode in which a stripe-shaped groove reaching the substrate is formed in a current blocking layer formed on a semiconductor substrate to confine the injected current, and the groove width of the groove is reflected from the light emitting surface side. An edge emitting light emitting diode characterized in that a current injection region is limited by continuously narrowing it to the surface side.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9220787A JPH077848B2 (en) | 1987-04-14 | 1987-04-14 | Edge emitting type light emitting diode |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9220787A JPH077848B2 (en) | 1987-04-14 | 1987-04-14 | Edge emitting type light emitting diode |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63257281A JPS63257281A (en) | 1988-10-25 |
| JPH077848B2 true JPH077848B2 (en) | 1995-01-30 |
Family
ID=14047997
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9220787A Expired - Lifetime JPH077848B2 (en) | 1987-04-14 | 1987-04-14 | Edge emitting type light emitting diode |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH077848B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP6220036B1 (en) * | 2016-11-30 | 2017-10-25 | 株式会社バンダイ | Model toy |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56142166A (en) * | 1979-10-25 | 1981-11-06 | Shichifuku Shiyokuhin Kk | Molding vessel for sealing pack |
| SE8005957L (en) * | 1980-08-26 | 1982-02-27 | Rigello Pak Ab | CAP |
| JPS59162455U (en) * | 1983-04-15 | 1984-10-31 | 三笠産業株式会社 | bottle closure |
| JPS59186254U (en) * | 1983-05-31 | 1984-12-11 | 三笠産業株式会社 | bottle lid |
| JPS60260292A (en) * | 1984-06-06 | 1985-12-23 | Matsushita Electric Ind Co Ltd | speaker system |
-
1987
- 1987-04-14 JP JP9220787A patent/JPH077848B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63257281A (en) | 1988-10-25 |
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