JPH0373577A - Light emitting diode - Google Patents

Light emitting diode

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Publication number
JPH0373577A
JPH0373577A JP1210312A JP21031289A JPH0373577A JP H0373577 A JPH0373577 A JP H0373577A JP 1210312 A JP1210312 A JP 1210312A JP 21031289 A JP21031289 A JP 21031289A JP H0373577 A JPH0373577 A JP H0373577A
Authority
JP
Japan
Prior art keywords
layer
type
active layer
ingaasp
undoped
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
Application number
JP1210312A
Other languages
Japanese (ja)
Inventor
Emiko Okano
岡野 恵聖子
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
NEC Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by NEC Corp filed Critical NEC Corp
Priority to JP1210312A priority Critical patent/JPH0373577A/en
Publication of JPH0373577A publication Critical patent/JPH0373577A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To improve mass productivity and luminous efficiency of the title device by providing an InGaAsP layer having the same composition as that of an active layer and undoped on a boundary between a P-type InGaAsP active layer and an N-type InP clad layer, diffusing Zn in the active layer into the undoped layer during liquid phase epitaxial growth, and then forming an effective thickness of the active layer. CONSTITUTION:An N-type InP clad layer 2, an undoped InGaAsP layer 3, a P-type InGaAsP layer 4, a P-type InP clad layer 5 and a P-type InGaAsP cap layer 6 are sequentially formed on an N-type InP substrate, an oxide film 7 is further formed on the layer 6 except a circular region M, and a P-type side electrode 8 is then formed thereon. Here, Zn of P-type dopant in the layer 4 is diffused in the layer 3 during liquid phase epitaxial growth of the layer 2, 3, 4, 5, 6. In this case, a distance between the PN junction and the active layer can be largely shortened to improve confinement efficiency of carriers in the active layer, thereby improving the luminous efficiency of an element.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は発光ダイオードに関し、特にInP基板上に形
成した、I nP/I nGaAsPダブルヘテロ型発
光ダイオードの構造に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a light emitting diode, and more particularly to the structure of an InP/InGaAsP double hetero type light emitting diode formed on an InP substrate.

〔従来の技術〕[Conventional technology]

通信用に用いられるI nP/I nGaAsPダブル
へテロ型発光ダイオード(以下、素子と略記する)の中
で応答速度が速いことを特徴とする素子として、活性層
に5 X 101gcm−3以上の高濃度のP型ドーパ
ントを混入させて形成した素子がある。従来、上述の素
子は、第2図に示すようにN型InP基板1上に、濃度
がI X 1018cxi−’程度のN型InPクラッ
ド層2と、濃度が5X101gCal−’以上のZn(
亜鉛〉をドープしたI nGaAsP活性As上P型I
nPクラッド層5及びP型InGaAsPキャップ層6
を形成した構造を有し、またこれらの各半導体層は液相
エピタキシャル成長によって形成していた。
Among the InP/InGaAsP double hetero type light emitting diodes (hereinafter abbreviated as devices) used for communication, this device is characterized by a fast response speed, and is characterized by a high response speed of 5 x 101 gcm-3 or more in the active layer. There are devices formed by mixing a high concentration of P-type dopants. Conventionally, as shown in FIG. 2, the above-mentioned device has an N-type InP cladding layer 2 on an N-type InP substrate 1 with a concentration of about I x 1018cxi-' and a Zn(
Zinc doped I nGaAsP P-type I on active As
nP cladding layer 5 and P-type InGaAsP cap layer 6
Each of these semiconductor layers was formed by liquid phase epitaxial growth.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上述の従来の発光ダイオードは、InGaAsP活性層
3に高濃度のZnを混入させているため、活性層形成後
の液相エピタキシャル成長中にInGaAsP活性層4
中のZnがN型InPりラッド層2中に拡散し、N型I
n97971層2のうちのInGaAsP活性層4に近
い側の一部がP型に反転し、PN接合がN型InPクラ
ッド層2中に形成される。この結果、InGaAsP活
性層4中へのキャリアの閉じ込め効率が悪化し、素子の
発光効率が低下するという欠点があった。また、Znの
拡散をできるだけおさえるために活性層より上部のエピ
タキシャル層(P型クラッド層及びキャップ層〉の成長
をスパークリング法により短時間に終らせる方法もある
が、スパークリング法は、メルトの均一性が悪いために
、均一性の良いエピタキシャル層を得ることが困難であ
り、量産性に欠けていた。一方ZnのN型In9797
1層2への拡散を押えるために、N濃度を高濃度にする
方法もあるが、高濃度にドープされたInP層は、表面
に凹凸となるいわゆるテラスが発生する。特に2 X 
l □ ta備−、にドーピングされたInP層のテラ
スの段差は大きい、そして、この凸部のInPはInP
中のP(リン)が解離しやすく、例えばテラスの激しい
InPクラッド層上に活性層を形成した場合、InP中
のPが解離した部分より活性層中に転位が発生し、素子
の寿命に重大の支障をきたすという欠点があった。
In the conventional light emitting diode described above, since a high concentration of Zn is mixed into the InGaAsP active layer 3, the InGaAsP active layer 4 is mixed during liquid phase epitaxial growth after forming the active layer.
The Zn inside diffuses into the N-type InP layer 2, and the Zn becomes the N-type I
A part of the n97971 layer 2 on the side closer to the InGaAsP active layer 4 is inverted to P type, and a PN junction is formed in the N type InP cladding layer 2. As a result, the efficiency of confining carriers in the InGaAsP active layer 4 deteriorates, resulting in a disadvantage that the light emitting efficiency of the device decreases. In addition, in order to suppress the diffusion of Zn as much as possible, there is a method in which the growth of the epitaxial layer (P-type cladding layer and cap layer) above the active layer is completed in a short time using the sparkling method. This made it difficult to obtain an epitaxial layer with good uniformity and lacked mass productivity.On the other hand, Zn N-type In9797
In order to suppress the diffusion into layer 1 and layer 2, there is a method of increasing the N concentration, but a highly doped InP layer produces uneven surfaces, ie, so-called terraces. Especially 2X
The step of the terrace of the InP layer doped with l □ ta is large, and the InP of this convex part is InP
P (phosphorus) in the InP is easily dissociated, and for example, if an active layer is formed on an InP cladding layer with severe terraces, dislocations will occur in the active layer from the parts where P in InP has dissociated, which will be critical to the life of the device. It had the disadvantage of causing problems.

本発明は上述の問題点を解決し、量産性に富み、発光効
率の良い発光ダイオードを得ることを目的として、いる
The present invention aims to solve the above-mentioned problems and provide a light-emitting diode that can be easily mass-produced and has good luminous efficiency.

〔課題を解決するための手段〕[Means to solve the problem]

本発明の発光ダイオードは、N型InP基板上にN型I
nPクラッド層と、アンドープでかつ活性層と同じ組成
をもつInGaAsP層、不純物濃度が5 X I Q
 18c11−3以上のP型InGaAsP活性層、P
型InPクラッド層およびP型InGaAsPキャップ
層を順次積層した構造を有している。
The light emitting diode of the present invention has an N-type I on an N-type InP substrate.
An nP cladding layer, an undoped InGaAsP layer with the same composition as the active layer, and an impurity concentration of 5
P-type InGaAsP active layer of 18c11-3 or higher, P
It has a structure in which an InP type cladding layer and a P type InGaAsP cap layer are sequentially laminated.

〔実施例〕〔Example〕

次に、本発明について図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.

第1図に、本発明の第1の実施例の素子の断面図を示す
FIG. 1 shows a sectional view of a device according to a first embodiment of the present invention.

本発明の第1の実施例の素子は、N型InP基板1上に
厚さ1μm、濃度I X 10 ”cm’″SのN型I
n97971層2、厚さ0.3μmのアンドープのI 
nGaAsP層3、厚さ0.3.czm、不純物濃度1
×1019cm−5のP型I nGaAsP活性層4、
厚さ1μm、不純物濃度5 X I O”CI+−’の
P型InPクラッド層5、及び厚さ1.5μm、不純物
濃度5 X I O18cm−’のP型InGaAsP
キャップ層6を順次形成し、さらに円形領域Mを除いた
P型InGaAsPキャップ層6の表面に酸化膜7を形
成し、続いて、その上に全面!@(P側電極)8を形成
し、また少なくとも円形領域Mの下に対応する円形領域
Nを除いたN型InP基板1の表面にN側電極Pを形成
した構造を有している。
The device of the first embodiment of the present invention has an N-type I layer on an N-type InP substrate 1 with a thickness of 1 μm and a concentration of I x 10 "cm'"S.
n97971 layer 2, undoped I with a thickness of 0.3 μm
nGaAsP layer 3, thickness 0.3. czm, impurity concentration 1
×1019 cm-5 P-type InGaAsP active layer 4,
A P-type InP cladding layer 5 with a thickness of 1 μm and an impurity concentration of 5 X I O"CI+-', and a P-type InGaAsP with a thickness of 1.5 μm and an impurity concentration of 5 X I O 18 cm-'
A cap layer 6 is sequentially formed, and then an oxide film 7 is formed on the surface of the P-type InGaAsP cap layer 6 except for the circular region M, and then the entire surface is covered with the oxide film 7! @(P-side electrode) 8 is formed, and the N-side electrode P is formed on the surface of the N-type InP substrate 1 excluding at least the circular region N corresponding to the bottom of the circular region M.

本素子は、上下を反対にして、N型InP基板側を上に
してヒートシンクにマウントして使用する。したがって
電流は電極8よりP型I nGaAsPキャップ層6、
P型InPクラッド層5、P型TnGaAsP活性層4
、アンドープInGaAsP層3、N型In97971
層2、及びN型基板1を経て電極9へ流れることとなる
。−方P型I nGaAsP活性層4で発生した光は、
N型In97971層2、N型InP基板1を経て、円
形領域Nより外部へ放射されることとなる。
This device is used by being turned upside down and mounted on a heat sink with the N-type InP substrate side facing up. Therefore, the current flows from the electrode 8 to the P-type InGaAsP cap layer 6,
P-type InP cladding layer 5, P-type TnGaAsP active layer 4
, undoped InGaAsP layer 3, N-type In97971
It will flow to the electrode 9 via the layer 2 and the N-type substrate 1. - The light generated in the P-type InGaAsP active layer 4 is
The light passes through the N-type In97971 layer 2 and the N-type InP substrate 1, and is radiated to the outside from the circular region N.

ここで、上述の素子における各半導体層2゜3.4,5
.6は液相エピタキシャル成長によって形成されたもの
であるが、成長中にI nGaAsP活性As中のP型
ドーパントであるZnがアンドープInGaAsP層3
に拡散する。従来、このPN接合と活性層の間の距離は
0.4μm程度であったが、本実施例では、活性層4を
0.3μmとし、アンドープのInGaAsP層3を0
.3μm設けることにより、0.01μm以下と大幅に
縮小することができ、この結果活性層中のキャリアの閉
じ込め効率が向上し、素子の発光効率は従来の約1.2
倍に向上した。
Here, each semiconductor layer 2°3.4,5
.. 6 is formed by liquid phase epitaxial growth, and during the growth, Zn, which is a P-type dopant in InGaAsP active As, forms an undoped InGaAsP layer 3.
spread to. Conventionally, the distance between this PN junction and the active layer was about 0.4 μm, but in this example, the active layer 4 was set to 0.3 μm, and the undoped InGaAsP layer 3 was set to 0.3 μm.
.. By providing 3 μm, the size can be significantly reduced to 0.01 μm or less, and as a result, the carrier confinement efficiency in the active layer is improved, and the luminous efficiency of the device is reduced to approximately 1.2 μm compared to the conventional one.
improved twice.

次に、本発明の第2の実施例の素子について説明する。Next, a device according to a second embodiment of the present invention will be explained.

第3図は、本発明第2の実施例の素子の断面図である。FIG. 3 is a sectional view of a device according to a second embodiment of the present invention.

同図に示すように第2の実施例の素子は、第1の実施例
に対し、P型I nGaAsP活性層4の層厚が0.1
μm、アンドープInGaAsP層3の層厚が0.5μ
mと薄くしたこと、さらにN側電極9をN型1nP基板
1の表面全面に形成したことの他は第1の実施例と同様
の素子構造となっている。すなわち、第1の実施例の素
子は、いわゆる面発光ダイオードであったのに対し、こ
の第2の実施例の素子は、光が活性層端面10より直接
外部に放射される端面発光ダイオードである。
As shown in the figure, in the device of the second embodiment, the layer thickness of the P-type InGaAsP active layer 4 is 0.1% different from that of the first embodiment.
μm, and the layer thickness of the undoped InGaAsP layer 3 is 0.5 μm.
The device structure is the same as that of the first embodiment except that the thickness is made as thin as m and that the N-side electrode 9 is formed over the entire surface of the N-type 1nP substrate 1. That is, while the element of the first embodiment was a so-called surface emitting diode, the element of the second embodiment is an edge emitting diode in which light is emitted directly to the outside from the end face 10 of the active layer. .

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明の素子は、高濃度のP型I
 nGaAsP活性層とN型InPクラッド層との境界
にアンドープでかつ活性層と同じ組成のX nGaAs
P層を設け、この活性層厚と、アンドープInGaAs
P層厚は、Znの濃度による拡散距離の関係から、最適
化し、液相エピタキシャル成長中にP型活性層中のZn
がアンドープInGaAsP層へ拡散した後、有効な活
性層厚をもつ構造とすることにより、N型InPクラッ
ド層中へのZnの拡散を押えることができる。
As explained above, the device of the present invention has a high concentration of P-type I
Undoped X nGaAs having the same composition as the active layer is placed at the boundary between the nGaAsP active layer and the N-type InP cladding layer.
A P layer is provided, and the active layer thickness and undoped InGaAs
The P layer thickness is optimized from the relationship between the diffusion distance depending on the Zn concentration, and the Zn in the P-type active layer is
After diffusion of Zn into the undoped InGaAsP layer, by creating a structure with an effective active layer thickness, diffusion of Zn into the N-type InP cladding layer can be suppressed.

この結果、活性層中へのキャリアの閉じ込め効率が向上
し、従来の素子より発光効率を向上できる効果がある。
As a result, the efficiency of confining carriers in the active layer is improved, which has the effect of improving luminous efficiency compared to conventional elements.

また、本構造によれば、成長速度の遅いオーバーシード
法による均一性の高い成長法を用いることができ、量産
性の点からも優れた効果が得られる。
Further, according to the present structure, it is possible to use a highly uniform growth method using an overseeding method with a slow growth rate, and an excellent effect can be obtained from the viewpoint of mass production.

【図面の簡単な説明】[Brief explanation of drawings]

第1図及び第3図は本発明の一実施例の素子断面図、第
2図は従来の素子の断面図の一部である0図中において
、 1・・・N型InP基板、2・・・N型InPクラッド
層、3・・・アンドープInGaAsP層、4・・・P
型InGaAsP活性層、5−P型InPクラッド層、
6・・・P型InGaAsPキャップ層、7・・・酸化
膜、8・・・P側電極、9・・・N側電極を示す。
1 and 3 are cross-sectional views of a device according to an embodiment of the present invention, and FIG. 2 is a partial cross-sectional view of a conventional device. ...N-type InP cladding layer, 3...Undoped InGaAsP layer, 4...P
type InGaAsP active layer, 5-P type InP cladding layer,
6... P-type InGaAsP cap layer, 7... Oxide film, 8... P-side electrode, 9... N-side electrode.

Claims (1)

【特許請求の範囲】[Claims]  N型InP基板上にN型InPクラッド層と、不純物
濃度が5×10^1^8cm^−^3以上のP型InG
aAsP活性層およびP型InPクラッド層、InGa
AsPキャップ層を順次積層した構造を有する発光ダイ
オードにおいて、P型InGaAsP活性層とN型In
Pクラッド層の間に、アンドープでかつ活性層と同じ組
成を有するInPGaAsP層を設けた構造であること
を特徴とする発光ダイオード。
An N-type InP cladding layer on an N-type InP substrate and a P-type InG with an impurity concentration of 5 x 10^1^8 cm^-^3 or more
aAsP active layer and P-type InP cladding layer, InGa
In a light emitting diode having a structure in which AsP cap layers are sequentially stacked, a P-type InGaAsP active layer and an N-type In
A light emitting diode characterized in that it has a structure in which an undoped InPGaAsP layer having the same composition as the active layer is provided between P cladding layers.
JP1210312A 1989-08-14 1989-08-14 Light emitting diode Pending JPH0373577A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1210312A JPH0373577A (en) 1989-08-14 1989-08-14 Light emitting diode

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1210312A JPH0373577A (en) 1989-08-14 1989-08-14 Light emitting diode

Publications (1)

Publication Number Publication Date
JPH0373577A true JPH0373577A (en) 1991-03-28

Family

ID=16587330

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1210312A Pending JPH0373577A (en) 1989-08-14 1989-08-14 Light emitting diode

Country Status (1)

Country Link
JP (1) JPH0373577A (en)

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