JPH05167101A - Semiconductor light emitting element - Google Patents

Semiconductor light emitting element

Info

Publication number
JPH05167101A
JPH05167101A JP35164691A JP35164691A JPH05167101A JP H05167101 A JPH05167101 A JP H05167101A JP 35164691 A JP35164691 A JP 35164691A JP 35164691 A JP35164691 A JP 35164691A JP H05167101 A JPH05167101 A JP H05167101A
Authority
JP
Japan
Prior art keywords
layer
light
light emitting
semiconductor
substrate
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.)
Granted
Application number
JP35164691A
Other languages
Japanese (ja)
Other versions
JP3152708B2 (en
Inventor
Kazumi Unno
和美 海野
Hideki Nozaki
秀樹 野崎
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP35164691A priority Critical patent/JP3152708B2/en
Publication of JPH05167101A publication Critical patent/JPH05167101A/en
Application granted granted Critical
Publication of JP3152708B2 publication Critical patent/JP3152708B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/819Bodies characterised by their shape, e.g. curved or truncated substrates
    • H10H20/82Roughened surfaces, e.g. at the interface between epitaxial layers
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/816Bodies having carrier transport control structures, e.g. highly-doped semiconductor layers or current-blocking structures

Landscapes

  • Led Devices (AREA)

Abstract

PURPOSE:To provide a semiconductor light emitting element which can effectively utilize light by improving its light emitting efficiency. CONSTITUTION:The title light emitting element has a light scattering layer 10 formed on the surface of the element on the side from which the light is taken out from a light emitting layer 2. The light scattering layer 10 is formed on the surface of a current diffusing layer 3 formed on the light emitting layer 2 by using a material having a lattice constant which is different from that the layer 3 has. After the layer 10 is grown on the layer 3, the surface of the layer 10 is roughened.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、輝度を高くした構造を
有する半導体発光素子に関するもので、とくに表示用光
源、例えば駅構内など屋内用情報表示板や、屋外のビル
広告板や道路の表示板、自動車のストップランプ、信号
機などに使用される半導体発光素子に関するものであ
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor light emitting device having a structure with increased brightness, and more particularly to a display light source, for example, an indoor information display board such as a station yard, an outdoor building advertisement board or a road display. The present invention relates to a semiconductor light emitting element used for a board, a stop lamp of an automobile, a traffic signal, and the like.

【0002】[0002]

【従来の技術】半導体結晶を用いた発光素子としては、
発光ダイオ−ド(LED、Light Emitting Diode)、レ
−ザダイオ−ド(LD、Laser Diode )、エレクトロル
ミネッセンス(EL、Electro-Luminescence)等が知ら
れている。前二者は、半導体接合に順方向電圧をかけ、
少数キャリアを注入して接合部で多数キャリアとの再結
合を起こし、このとき放出される光を利用する素子であ
る。エレクトロルミネッセンスは、結晶体に電界を加え
たときに発光する現象である。印加電圧としては直流、
交流いずれでも可能である。これら半導体発光素子の中
でも発光ダイオ−ド、とくに、高輝度のLEDは、表示
用光源、たとえば屋内や駅構内用情報表示板、道路表示
用情報板、自動車のストップランプ、信号機等に使用さ
れている。また、低電流でも高輝度であるために従来よ
りも省エネルギ−タイプの表示用光源として用いられ
る。このような分野に使用されるLEDとしては次のよ
うなものがある。まず、赤色発光素子としては、ピ−ク
波長が630nm程度のGaAsP赤色LEDおよびピ
−ク波長が660nm程度のGaAlAs赤色LEDが
あり、橙色発光素子としては、ピ−ク波長が610nm
程度のGaAsP橙色LED、黄色発光素子としては、
ピ−ク波長が590nm程度のGaAsP黄色LED
が、更に緑色発光素子としては、ピ−ク波長が565n
m程度のGaP緑色LEDが用いられている。各々の素
子の輝度は、GaAsPLEDで300mcd前後、G
aAlAs赤色LEDではシングルヘテロ(SH)構造
の場合、500mcd前後、GaAs基板を取り除いた
型のダブルヘテロ(DH)構造の場合3000mcd前
後、GaP緑色LEDでは500mcd前後が得られて
いる。なお、半導体発光素子を形成する主な手段として
は、厚膜形成法として周知のエピタキシャル結晶成長法
である気相成長法(VPE)や液相成長法(LPE)が
知られており、VPEは、GaAsPの形成、LPE
は、GaAlAs、GaP等の形成にそれぞれ適してい
る。その他に有機金属を用いたVPE(MOVPEMeta
l Organic Vapour Phase Epitaxy)やMBE(Molecula
r Beam Epitaxy)などの方法が知られている。
2. Description of the Related Art As a light emitting device using a semiconductor crystal,
Light emitting diodes (LEDs, Light Emitting Diodes), laser diodes (LDs, Laser Diodes), electroluminescence (EL, Electro-Luminescence) and the like are known. The former two apply a forward voltage to the semiconductor junction,
In this device, minority carriers are injected to cause recombination with majority carriers at the junction, and the light emitted at this time is used. Electroluminescence is a phenomenon in which light is emitted when an electric field is applied to a crystal body. The applied voltage is direct current,
Either exchange is possible. Among these semiconductor light emitting devices, a light emitting diode, in particular, a high-brightness LED is used as a display light source, for example, an information display board for indoors or in stations, a road display information board, an automobile stop lamp, and a traffic signal. There is. Further, since it has high brightness even at low current, it is used as an energy-saving type display light source as compared with the conventional one. The LEDs used in such fields are as follows. First, as the red light emitting element, there are GaAsP red LED having a peak wavelength of about 630 nm and GaAlAs red LED having a peak wavelength of about 660 nm, and as the orange light emitting element, a peak wavelength is 610 nm.
About GaAsP orange LED and yellow light emitting element,
GaAsP yellow LED with peak wavelength of about 590 nm
However, as a green light emitting element, the peak wavelength is 565n.
GaP green LEDs of about m are used. The brightness of each element is about 300 mcd for GaAsPLED, G
The aAlAs red LED has a single hetero (SH) structure of about 500 mcd, the double hetero (DH) structure without the GaAs substrate has a structure of about 3000 mcd, and the GaP green LED has a structure of about 500 mcd. As a main means for forming a semiconductor light emitting element, a vapor phase growth method (VPE) or a liquid phase growth method (LPE), which is an epitaxial crystal growth method known as a thick film forming method, is known. , GaAsP formation, LPE
Are suitable for forming GaAlAs, GaP, etc., respectively. In addition, VPE (MOVPEMeta using organic metal)
l Organic Vapor Phase Epitaxy) and MBE (Molecula)
r Beam Epitaxy) and other methods are known.

【0003】従来技術の一例を図5により説明する。半
導体基板1には、不純物濃度が3×1018cm-3程度の
n−GaAs基板を用いる。このn−GaAs基板1上
に、厚さ1μm、不純物濃度5×1017cm-3のn−I
0.5 (Ga1-x Alx 0.5 Pクラッド層21、厚さ
0.6μmのアンドープIn0.5 (Ga1-y Aly
0.5 P活性層20、厚さ1μm、不純物濃度5×1017
cm-3のp−In0.5 (Ga1-z Alz 0.5 Pクラッ
ド層22、さらに、厚さ7μm、不純物濃度1×1018
cm-3のp−Ga1-u Alu As電流拡散層3を順次た
とえばMOVPE法で成長させる。次に、基板1の他の
表面には、例えば、Au−Geなどのn側電極4をオ−
ミックコンタクトさせ、反対側の電流拡散層3上には、
例えば、Au−Znなどのp側電極5をオ−ミックコン
タクトさせる。電流拡散層3であるGa1-u Alu As
層はp側電極5からの電流をLEDチップ全面に拡散さ
せるために設けられたものであるが、発光素子として必
ずしも必要ではなく、これを用いないものもある。図で
は、uが0.7の場合を示した。この層の存在によっ
て、活性層全域で発光させることが可能になるので、チ
ップからの光取出し効率を大幅に改善することができ
る。これらの各種成長層はGaAs基板と格子整合がと
れていることおよびダブルヘテロ構造であること、活性
層のyを0〜0.7まで変化させると約660nmの赤
色発光から約555nmの緑色発光の範囲で直接遷移型
バンド構造が得られことおよびダブルヘテロ構造を用い
ることなどにより高い発光効率が得られる。この例で
は、電流拡散層側から光が取り出されるので、p側電極
5が、光取出し側電極となる。光取出し側電極は、通常
ボンデイングパッドによって外部配線と接続されてい
る。
An example of the prior art will be described with reference to FIG. As the semiconductor substrate 1, an n-GaAs substrate having an impurity concentration of about 3 × 10 18 cm −3 is used. On this n-GaAs substrate 1, an n-I having a thickness of 1 μm and an impurity concentration of 5 × 10 17 cm −3 was formed.
n 0.5 (Ga 1-x Al x ) 0.5 P cladding layer 21, 0.6 μm thick undoped In 0.5 (Ga 1-y Al y ).
0.5 P active layer 20, thickness 1 μm, impurity concentration 5 × 10 17
cm −3 p-In 0.5 (Ga 1-z Al z ) 0.5 P cladding layer 22, further having a thickness of 7 μm and an impurity concentration of 1 × 10 18.
The cm −3 p-Ga 1 -u Al u As current diffusion layer 3 is sequentially grown by, for example, the MOVPE method. Next, on the other surface of the substrate 1, an n-side electrode 4 such as Au-Ge is opened.
Mic contact, and on the opposite side of the current diffusion layer 3,
For example, the p-side electrode 5 such as Au-Zn is brought into ohmic contact. Ga 1-u Al u As which is the current diffusion layer 3
The layer is provided for diffusing the current from the p-side electrode 5 over the entire surface of the LED chip, but it is not always necessary as a light emitting element, and some layers do not use it. The figure shows the case where u is 0.7. The presence of this layer enables light emission over the entire active layer, so that the light extraction efficiency from the chip can be significantly improved. These various growth layers are lattice-matched with the GaAs substrate and have a double hetero structure. When y of the active layer is changed from 0 to 0.7, red emission of about 660 nm to green emission of about 555 nm are emitted. High emission efficiency can be obtained by obtaining a direct transition band structure in the range and by using a double hetero structure. In this example, since the light is extracted from the current diffusion layer side, the p-side electrode 5 serves as the light extraction-side electrode. The light extraction side electrode is usually connected to an external wiring by a bonding pad.

【0004】なお、この種の発光素子において、発光に
直接寄与する部分は、活性層20とこの活性層を挟む1
対のクラッド層21、22であるので、ここでは、これ
らの層をまとめて発光層2と定義する。この素子は、発
光層2でのpn接合がダブルヘテロ構造であるが、以
下、シングルヘテロやホモ接合などの他の構造の素子の
場合でも発光に直接寄与する部分は発光層と称する。
In this type of light emitting device, the portion that directly contributes to light emission is sandwiched between the active layer 20 and this active layer 1.
Since the clad layers 21 and 22 are a pair, these layers are collectively defined as the light emitting layer 2 here. In this element, the pn junction in the light emitting layer 2 has a double hetero structure, but hereinafter, even in the case of an element having another structure such as a single hetero or a homo junction, a portion directly contributing to light emission is referred to as a light emitting layer.

【0005】ところで、例えば、屋外用の表示用光源の
場合、各々の発光色領域において1cd以上の輝度が必
要である。赤色領域では直接遷移型であるGaAlAs
LEDは1cd以上の輝度が容易に得られているが、赤
色より短波長領域では間接遷移型であるGaAsPLE
DやGaPLEDを使用しているため、500mcd程
度がほぼ限界とみられ、屋外用として十分に機能してい
ないのが現状である。したがって、これらの色のLED
を屋外用に使用する場合は、GaAlAs赤色LEDな
ら1個ですむところが、複数個使用せざるを得ないので
コストアップとなる。後述するように直接遷移型である
InGaAlPLEDにおいても十分な輝度が得られな
い。この原因の1つに、発光した光を有効に活用してい
ないことが挙げられる。前述した電流拡散層の存在によ
って、効率良く発光することは出来るが、その光を十分
生かすことができない。発光層2から出た光は、一部は
そのまま光取出し側の表面から外部へ出るが。一方、半
導体基板が透明な場合反対側の下方へ向かった光はn側
電極を、例えば、水玉形状にしておけば、水玉電極以外
の所の基板表面で反射され、上方の光取出し側表面から
外部へ出て、また、基板の側面からも光が外部に放射さ
れるので、下方に向かった光も有効に外部に取り出すこ
とができる。
By the way, for example, in the case of an outdoor display light source, a luminance of 1 cd or more is required in each emission color region. GaAlAs, which is a direct transition type in the red region
Although LEDs with a brightness of 1 cd or more are easily obtained, GaAsPLE is an indirect transition type in the wavelength range shorter than red.
Since D and GaPLED are used, the limit is about 500 mcd, and the current situation is that they do not function sufficiently for outdoor use. Therefore, LEDs of these colors
When using the LED for outdoor use, only one GaAlAs red LED is required, but it is necessary to use a plurality of LEDs, which increases the cost. As will be described later, sufficient brightness cannot be obtained even in the InGaAlPLED which is a direct transition type. One of the causes is that the emitted light is not effectively used. Due to the presence of the current diffusion layer described above, light can be efficiently emitted, but the light cannot be fully utilized. A part of the light emitted from the light emitting layer 2 goes out from the surface on the light extraction side as it is. On the other hand, when the semiconductor substrate is transparent, the light traveling downward on the opposite side is reflected on the substrate surface other than the polka dot electrode if the n-side electrode is shaped like a polka dot, and is reflected from the upper light extraction side surface. Since light is emitted to the outside and is also emitted to the outside from the side surface of the substrate, the light directed downward can be effectively extracted to the outside.

【0006】しかし、例えば、発光層における活性層と
してバンドギャップの大きいInGaAlP系混晶半導
体を用いた発光素子を考えると、半導体基板1がバンド
ギャップの小さいGaAs等の材料の場合、発光層は短
波長を発光するので、発せられる光の多くはこの基板に
吸収されてしまう。したがって下方に向かった光は、外
部に取り出すことは出来ない。そのため半導体基板に
は、光吸収の少ないものを選ばなければならないので、
材料が限定されてしまう。従来は、半導体基板による光
の吸収を防いで、発光効率を上げると同時に基板材料の
選択の範囲を広げるために、発光層と半導体基板の間に
光反射層を形成していた。発光層2から出た光は、下方
の半導体基板1の方向に向かっても、この光反射層によ
って反射されて半導体基板による光の吸収は防がれる。
この光反射層は、例えば、発光層の直下に屈折率の異な
る二種類以上の物質を、光の波長の1/4倍相当もしく
はこれに比例した相当の厚さに交互に積層して形成す
る。電流拡散層としては、Ga1-u Alu As層が良く
知られている材料である。一方、光反射層を設けずに下
方に向った光を外部に取り出す方法としては例えばGa
As基板の代りにGaP基板を使用したIuGaAlP
−LEDがある。GaP基板はInGaAlP−LED
の発光色(緑色〜赤色)に対して透明なため反射層を設
ける必要はない。しかしこの場合はGaP基板とIn
0.5 (Ga1-x Alx 0.5 Pとの格子不整合による格
子欠陥が多発するため発光効率が低下し効果的に輝度の
高いLEDが得られない。この対策としてIn0.5 (G
1-x Alx 0.5 Pを成長させる前に先ずGaP基板
上に組成比が少しずつ変化するIn1-v Gav P組成勾
配層(v=1→0.5)を成長させることによりGaP
基板とIn0.5 (Ga1-x Alx 0.5 Pとの間の格子
定数の違いを吸収させる方法がとられている。In1-v
Gav P組成勾配層の代りにIn1-v (Ga1-w
w v P組成勾配層(v=1→0.5)としても良
い。また、発光層と光取出し電極の間に光反射層を設け
て、光取出し電極によって反射された光を有効に取り出
すようにした半導体発光素子も、本発明の発明者等によ
って開発されている(特願平3−163359号)。
However, considering a light emitting element using an InGaAlP mixed crystal semiconductor having a large band gap as an active layer in the light emitting layer, when the semiconductor substrate 1 is made of a material such as GaAs having a small band gap, the light emitting layer is short. Since it emits a wavelength, most of the emitted light is absorbed by this substrate. Therefore, the light directed downward cannot be extracted to the outside. For that reason, it is necessary to select a semiconductor substrate that absorbs less light.
Materials are limited. Conventionally, a light reflecting layer is formed between a light emitting layer and a semiconductor substrate in order to prevent light from being absorbed by the semiconductor substrate, improve luminous efficiency, and at the same time widen the range of substrate material selection. The light emitted from the light emitting layer 2 is reflected by this light reflecting layer even in the direction of the semiconductor substrate 1 below, and the absorption of light by the semiconductor substrate is prevented.
This light reflection layer is formed, for example, by directly laminating two or more kinds of substances having different refractive indexes directly below the light emitting layer to a thickness equivalent to ¼ times the wavelength of light or an equivalent thickness. .. A Ga 1-u Al u As layer is a well-known material for the current spreading layer. On the other hand, as a method of extracting the light directed downward without providing the light reflection layer, for example, Ga is used.
IuGaAlP using GaP substrate instead of As substrate
-There is an LED. GaP substrate is InGaAlP-LED
Since it is transparent to the emission color (green to red), it is not necessary to provide a reflective layer. However, in this case, the GaP substrate and the In
Since many lattice defects occur due to lattice mismatch with 0.5 (Ga 1-x Al x ) 0.5 P, the luminous efficiency is reduced and an LED with high brightness cannot be obtained effectively. In 0.5 (G
By a 1-x Al x) composition ratio on first GaP substrate before growing 0.5 P is grown the In 1-v Ga v P gradient composition layer gradually changes (v = 1 → 0.5) GaP
A method of absorbing a difference in lattice constant between the substrate and In 0.5 (Ga 1-x Al x ) 0.5 P is adopted. In 1-v
Instead of the Ga v P composition gradient layer, In 1-v (Ga 1-w A
1 w ) v P composition gradient layer (v = 1 → 0.5). The inventors of the present invention have also developed a semiconductor light emitting device in which a light reflection layer is provided between the light emitting layer and the light extraction electrode to effectively extract the light reflected by the light extraction electrode ( Japanese Patent Application No. 3-163359).

【0007】[0007]

【発明が解決しようとする課題】以上のように、活性層
と半導体基板との間、もしくは、光取出し側電極と活性
層との間に挿入された光反射層および電流拡散層の存在
によって発光効率は上がり、光の利用率も向上するが、
まだ橙色から緑色までの範囲で1cd以上のLEDを得
るに十分とはいえない。またGaP基板上にIn1-v
v P組成勾配層またはIn1-v (Ga1-w Alw v
P組成勾配層を成長させてから発光層を形成する方法に
よっても光の利用率は向上するが、この場合GaP基板
とIn0.5 (Ga1-x Alx 0.5 Pとの間の格子定数
の違いを完全には吸収することができず、そのため結晶
欠陥が多くなって内部発光効率が低下し、結果的には1
cd以上のLEDが得られない。
As described above, light is emitted due to the presence of the light reflection layer and the current diffusion layer inserted between the active layer and the semiconductor substrate or between the electrode on the light extraction side and the active layer. Efficiency goes up and light utilization goes up, but
It is still not sufficient to obtain LEDs of 1 cd or more in the range from orange to green. In 1-v G on the GaP substrate
a v P composition gradient layer or In 1-v (Ga 1-w Al w ) v
The light utilization rate is also improved by the method of growing the P composition gradient layer and then forming the light emitting layer, but in this case, the lattice constant of the lattice constant between the GaP substrate and In 0.5 (Ga 1-x Al x ) 0.5 P is increased. The difference cannot be completely absorbed, so that the number of crystal defects increases and the internal luminous efficiency decreases, resulting in 1
LED of more than cd cannot be obtained.

【0008】本発明は、以上のような事情によってなさ
れたものであり、発光効率を上げて光を有効に利用する
ことができる半導体発光素子、例えば、InGaAlP
四元系混晶を用いた場合のように短波長の光が発する材
料を活性層に用いて輝度が1cd以上になるようなLE
Dを提供することを目的としている。
The present invention has been made under the above circumstances, and is a semiconductor light emitting device capable of increasing light emission efficiency and effectively utilizing light, for example, InGaAlP.
LE having a brightness of 1 cd or more by using a material that emits light of a short wavelength as an active layer as in the case of using a quaternary mixed crystal
It is intended to provide D.

【0009】[0009]

【課題を解決するための手段】本発明の半導体発光素子
は、活性層を含む発光層と、この発光層の上に形成さ
れ、光取出し面を有する光散乱層と、前記発光層もしく
は前記光散乱層の上に形成された光取出し側電極とを備
えていることを第1の特徴としている。また、活性層を
含む発光層と、この発光層の上に形成された電流拡散層
と、この電流拡散層の上に形成され、光取出し面を有す
る光散乱層と、前記電流拡散層もしくは前記光散乱層の
上に形成された光取出し側電極とを備えていることを第
2の特徴としている。前記発光層は、シングルヘテロ接
合、ダブルヘテロ接合もしくはホモ接合のいずれかを備
えている。前記発光層がInGaAlP系混晶半導体を
活性層として備えている半導体発光素子において、前記
光散乱層はGaP、ZnS、ZnSeおよびZnSe−
ZnSから選ばれる材料を用いることができる。前記光
散乱層の厚さは、0.5μm以上であり、その光散乱層
の半導体結晶の格子定数は、その底面と接する半導体結
晶の格子定数とは0.3%以上異なるようにすることが
できる。前記発光層の前記光散乱層が形成されている面
とは反対側の表面には、半導体基板が設けられ、この半
導体基板の前記発光層が形成されている面とは反対側の
表面には、基板側電極が設けられており、前記半導体基
板のバンドギャップが、前記活性層のバンドギャップと
ほぼ同じか、あるいはそれより大きいバンドギャップを
有するように半導体基板材料を選ぶ場合は、前記基板側
電極は、水玉模様の形状にすることができる。さらに、
前記光取出し側電極の直下には光反射層を形成すること
も可能である。
A semiconductor light emitting device of the present invention comprises a light emitting layer including an active layer, a light scattering layer formed on the light emitting layer and having a light extraction surface, the light emitting layer or the light emitting layer. The first feature is that the light extraction side electrode is formed on the scattering layer. In addition, a light emitting layer including an active layer, a current diffusion layer formed on the light emitting layer, a light scattering layer formed on the current diffusion layer and having a light extraction surface, the current diffusion layer or the The second characteristic is that the light extraction side electrode is formed on the light scattering layer. The light emitting layer has a single heterojunction, a double heterojunction, or a homojunction. In the semiconductor light emitting device in which the light emitting layer includes an InGaAlP-based mixed crystal semiconductor as an active layer, the light scattering layer includes GaP, ZnS, ZnSe, and ZnSe-.
A material selected from ZnS can be used. The thickness of the light scattering layer is 0.5 μm or more, and the lattice constant of the semiconductor crystal of the light scattering layer is different from the lattice constant of the semiconductor crystal in contact with the bottom surface by 0.3% or more. it can. A semiconductor substrate is provided on the surface of the light emitting layer opposite to the surface on which the light scattering layer is formed, and on the surface of the semiconductor substrate opposite to the surface on which the light emitting layer is formed. When the semiconductor substrate material is selected such that the substrate side electrode is provided and the band gap of the semiconductor substrate is substantially the same as or larger than the band gap of the active layer, the substrate side is selected. The electrodes can be polka dot shaped. further,
It is also possible to form a light reflection layer directly below the light extraction side electrode.

【0010】[0010]

【作用】発光層から光取出し面に向った光は、光散乱層
の光散乱面の効果により光が外部に出やすくなり、また
発光層の下側に反射層がある場合は、発光層から反射層
に向った光は反射層で反射し、光取出し面に向い、光散
乱面の効果により、より多くの光が外部に出る。この光
散乱層の効果を例えば光取出し面が鏡面の場合(InG
aAlP−LEDの場合、通常は、鏡面となっている)
と比較すると次のようになる。今、光取出し面の下の結
晶の屈折率をn、空気の屈折率を1とすると、鏡面の場
合光取出し効率ηc は、ηc =1/2[1−cos(s
in-11/n)][1−(n−1/n+1)2 ]とあら
わされ、n=3.4とすると、ηc =0.0155=
1.55%となる。また完全光散乱面の場合のηc は、
ηc=1/2(1/n)2 f(n)とあらわされ、n=
3.4の時、f(n)=0.685であるから、ηc
0.0296=2.96%となる。ここでは、光は発光
層から光取出し面側(上方)とその反対側(下方)に放
射され下方に向った光は完全吸収すると仮定した。上式
の計算結果から分るように、光取出し面が光散乱層に形
成されている方が光取出し効果が約2倍向上する。発光
層の下側に反射層を設けた場合も、光取出し電極の直下
に光反射層を設けた場合も同様な効果が得られる。
[Function] The light emitted from the light emitting layer toward the light extraction surface is easily emitted to the outside due to the effect of the light scattering surface of the light scattering layer, and when the reflection layer is below the light emitting layer, the light is emitted from the light emitting layer. Light directed to the reflective layer is reflected by the reflective layer and directed to the light extraction surface, and more light is emitted to the outside due to the effect of the light scattering surface. The effect of this light scattering layer is, for example, when the light extraction surface is a mirror surface (InG
In the case of aAlP-LED, it is usually a mirror surface)
Compared with Assuming that the refractive index of the crystal below the light extraction surface is n and the refractive index of air is 1, the light extraction efficiency η c in the case of a mirror surface is η c = 1/2 [1-cos (s
in −1 1 / n)] [1- (n−1 / n + 1) 2 ], where n = 3.4, η c = 0.0155 =
It becomes 1.55%. In the case of a perfect light scattering surface, η c is
η c = 1/2 (1 / n) 2 f (n), where n =
At the time of 3.4, since f (n) = 0.685, η c =
It becomes 0.0296 = 2.96%. Here, it is assumed that light is emitted from the light emitting layer to the light extraction surface side (upper side) and the opposite side (lower side), and the light directed downward is completely absorbed. As can be seen from the calculation result of the above equation, the light extraction effect is improved about twice when the light extraction surface is formed in the light scattering layer. Similar effects can be obtained when the reflective layer is provided below the light emitting layer and when the light reflective layer is provided immediately below the light extraction electrode.

【0011】[0011]

【実施例】以下、本発明の実施例を図面を参照して説明
する。図1は、第1の実施例に係る半導体発光素子であ
る発光ダイオードの概略構造を示す断面図である。図示
のように、基本的構造は、一方の電極を有する化合物半
導体基板1と、この基板上の光反射層6、発光層2、電
流拡散層3、光散乱層10及び光取出し側電極5とを含
んでいる。光反射層によって基板による光吸収をできる
だけ回避し、光散乱層によって光が外部へ出る率を向上
させる。図において化合物半導体基板1は、n−GaA
sを用いる。この基板1上に、発光波長の1/2程度の
厚さのn−InAlPとn−InGaAlPとが交互に
積層された多層構造の光反射層6が成長形成されてい
る。この光反射層6の上にはn−InAlPクラッド層
21、InGaAlP活性層20およびp−InAlP
クラッド層22から構成されるダブルヘテロ構造の発光
層2が成長形成されている。このp−InAlPクラッ
ド層22上に、電流が発光層全体に流れるようにして発
光層全域で発光させるためのp−GaAlAs電流拡散
層3が成長形成されている。さらに、この電流拡散層3
上に、本発明の特徴である光散乱層(この実施例では、
P−GaP層)10が成長形成されている。また、基板
1側には、n側オーミック電極7(基板側電極)が形成
され、光散乱層10側にはp型オーミック電極(光取出
側電極)5が形成されている。このp側オーミック電極
5は通常のフォトエッチングにより所定の形状に形成さ
れる。図1の例では、光散乱層10の表面が粗面のた
め、光取出し電極(p側オ−ミック電極)のみ光散乱層
10をエッチング除去している。しかし、光散乱層10
の上に直接光取出し電極を形成することもできる。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a sectional view showing a schematic structure of a light emitting diode which is a semiconductor light emitting element according to the first embodiment. As shown in the figure, the basic structure includes a compound semiconductor substrate 1 having one electrode, a light reflection layer 6, a light emitting layer 2, a current diffusion layer 3, a light scattering layer 10 and a light extraction side electrode 5 on this substrate. Is included. The light reflection layer avoids light absorption by the substrate as much as possible, and the light scattering layer improves the rate of light out. In the figure, the compound semiconductor substrate 1 is n-GaA.
s is used. On this substrate 1, a light reflection layer 6 having a multi-layer structure in which n-InAlP and n-InGaAlP having a thickness of about ½ of the emission wavelength are alternately laminated is grown. An n-InAlP cladding layer 21, an InGaAlP active layer 20 and a p-InAlP layer are formed on the light reflection layer 6.
The light emitting layer 2 having a double hetero structure composed of the cladding layer 22 is grown and formed. On the p-InAlP clad layer 22, a p-GaAlAs current diffusion layer 3 is grown and formed so that a current flows in the entire light emitting layer so that light is emitted in the entire light emitting layer. Furthermore, this current spreading layer 3
In addition, the light-scattering layer which is a feature of the present invention (in this embodiment,
A P-GaP layer) 10 is grown and formed. An n-side ohmic electrode 7 (substrate-side electrode) is formed on the substrate 1 side, and a p-type ohmic electrode (light-extraction-side electrode) 5 is formed on the light-scattering layer 10 side. The p-side ohmic electrode 5 is formed into a predetermined shape by ordinary photoetching. In the example of FIG. 1, since the surface of the light scattering layer 10 is rough, only the light extraction electrode (p-side ohmic electrode) is removed by etching. However, the light scattering layer 10
It is also possible to form the light extraction electrode directly on the above.

【0012】次に、上記半導体発光素子の製造方法につ
いて具体的に説明する。各半導体層は、有機金属化学気
相成長法(MOVPE法)により成長させた。原料には
トリメチルインジウム(TMI)、トリメチルガリウム
(TMG)、トリメチルアルミニウム(TMA)をIII
族元素のソースとして、アルシン(AsH3 )とフォス
フィン(PH3 )をV族元素のソースとして用いた。ま
たP型ドーパントとしてZn、n型ドーパントとしてS
iを用いたが、これらはそれぞれジメチル亜鉛(DM
Z)、シラン(SiH4 )をソースとしてドープした。
この反応性ガスを水素をキャリアガスとして石英製反応
管に輸送して、SiCコーティングしたグラファイトサ
セプタ上に設置したn−GaAs基板に結晶成長させ
た。反応管内部の圧力は30〜100Torrであり、
基板は800℃程度に加熱される。n−GaAs基板に
はSiをドープし、キャリア濃度は3×1018cm-3
度のものを用いた。基板の面方位は(100)である。
初めに、n−GaAs基板1上に、n−In0.5 Al
0.5 Pとn−In0.5 Ga0.2 Al0.3 Pを交互に複数
積層して構成された光反射層6を4.3μm程度成長さ
せる。各半導体層は、Siドープされ、キャリア濃度1
×1018cm-3であり、光を効率よく反射するために発
光波長の約1/2(約86nm)の積層周期で交互に積
層する。ついで、この光反射層6上に、厚さ1μmのn
−In0.5 Al0.5 P(Siドープ、キャリア濃度5×
1017cm-3)21、厚さ0.6μmのアンドープIn
0.5 Ga0.21Al0.29P活性層20、p−In0.5 Al
0.5 P(Znドープ、キャリア濃度5×1017cm-3
クラッド層22からなるダブルヘテロ構造の発光層2を
形成する。その後、発光波長に対して透明なp−Ga
0.2 Al0.8As(Znドープ、4×1018cm-3)電
流拡散層3を7μm程度成長させる。つぎに、Znをド
−プした不純物濃度4×1018/cm3 のp−GaP光
散乱層10を1μm程度成長させる。p−GaPの格子
定数は、GaAlAsの格子定数と同じでないため格子
不整合による不完全成長になるので、p−GaP成長面
は、粗面となり、光散乱層が形成される。
Next, a method for manufacturing the above semiconductor light emitting device will be specifically described. Each semiconductor layer was grown by a metal organic chemical vapor deposition method (MOVPE method). Trimethyl indium (TMI), trimethyl gallium (TMG), and trimethyl aluminum (TMA) are used as raw materials.
Arsine (AsH 3 ) and phosphine (PH 3 ) were used as sources of group V elements as sources of group V elements. Zn as a P-type dopant and S as an n-type dopant
i was used, and these are dimethyl zinc (DM
Z) and silane (SiH 4 ) as a source.
This reactive gas was transported to a quartz reaction tube using hydrogen as a carrier gas, and crystal growth was performed on an n-GaAs substrate placed on a SiC-coated graphite susceptor. The pressure inside the reaction tube is 30 to 100 Torr,
The substrate is heated to about 800 ° C. The n-GaAs substrate was doped with Si and had a carrier concentration of about 3 × 10 18 cm -3 . The plane orientation of the substrate is (100).
First, on the n-GaAs substrate 1, n-In 0.5 Al
A light-reflecting layer 6 formed by alternately laminating a plurality of 0.5 P and n-In 0.5 Ga 0.2 Al 0.3 P is grown to a thickness of about 4.3 μm. Each semiconductor layer is Si-doped and has a carrier concentration of 1
It is × 10 18 cm -3 , and in order to reflect light efficiently, the layers are alternately stacked at a stacking cycle of about ½ (about 86 nm) of the emission wavelength. Then, on the light reflection layer 6, n having a thickness of 1 μm is formed.
-In 0.5 Al 0.5 P (Si-doped, carrier concentration 5 ×
10 17 cm −3 ) 21, 0.6 μm thick undoped In
0.5 Ga 0.21 Al 0.29 P active layer 20, p-In 0.5 Al
0.5 P (Zn-doped, carrier concentration 5 × 10 17 cm −3 )
A light emitting layer 2 having a double hetero structure composed of the clad layer 22 is formed. Then, p-Ga which is transparent to the emission wavelength
A 0.2 Al 0.8 As (Zn-doped, 4 × 10 18 cm −3 ) current diffusion layer 3 is grown to about 7 μm. Next, a Zn-doped p-GaP light-scattering layer 10 having an impurity concentration of 4 × 10 18 / cm 3 is grown to about 1 μm. Since the lattice constant of p-GaP is not the same as that of GaAlAs, imperfect growth due to lattice mismatch occurs, so the p-GaP growth surface becomes a rough surface and a light scattering layer is formed.

【0013】このようにして得られた緑色LED用ウェ
−ハに電極を形成するために、まずp−GaP光散乱層
10を、部分的にエッチング除去して光取出し電極(p
側電極)5を形成すべき部分を露出させる。つぎに、真
空蒸着法によりこのウェ−ハのn−GaAs基板1側に
AuGe合金層4を0.5μm、p−GaP光散乱層1
0側にAuBe合金層を0.3μm蒸着した後、480
℃、10分間、Ar雰囲気中でシンタして、オーミック
コンタクトを形成する。ついで、再び真空蒸着法により
このウェ−ハのAuBe合金層上に純金を1μm程度堆
積し、これを写真蝕刻法により先のp−GaP光散乱層
に形成したp−GaAlAs電流拡散層3の露出部のみ
を除いてAuBe合金層と純金層を取り除く。この様に
してp側電極5がp−GaAlAs電流拡散層3の光沢
面に形成される。このような複雑な工程を採用する理由
は、自動ワイヤボンデイング時の電極検出のために、電
極面が光沢を持つ必要があるからである。そして、最後
に所定のピッチでダイシングして個々のペレットに分離
する。このようにしてp側電極5側を光取出し側とする
高効率緑色LEDが完成する。このp側電極5が形成さ
れている面から発光層2で生じた光が外部に取出される
ので、この電極が光取出し側電極となる。すなわち、こ
のLEDでは、ダブルヘテロ構造部の活性層で発生した
光は、p側電極5側、基板1側及び側面に向かうことに
なる。基板1側に向う光は、光反射層6で効率よく反射
され、光取出し側に向い、その1部が、光取出し面から
取出され、またp型電極5へ向う光も同様にその1部が
光取出し面から取り出される。この時、素子の光取出し
面が光散乱層になっているために、従来の電流拡散層の
光沢面から光を取出す場合よりも約2倍光取出し効率が
向上して1cd以上の緑色LEDが実現する。このよう
に実施例によれば、特別な基板を用いなくても高品質で
安価なGaAs基板を使用した緑色領域で発光する高輝
度のLEDを作成することができる。低コストで緑色L
EDが量産できることはディスプレイ、光通信等の情報
産業への貢献が極めて大であるといえる。
In order to form an electrode on the thus obtained green LED wafer, first, the p-GaP light scattering layer 10 is partially removed by etching to remove the light extraction electrode (p.
The portion where the side electrode) 5 is to be formed is exposed. Next, an AuGe alloy layer 4 of 0.5 μm and a p-GaP light-scattering layer 1 were formed on the n-GaAs substrate 1 side of this wafer by vacuum deposition.
480 after depositing a 0.3 μm AuBe alloy layer on the 0 side
Sintering is performed in an Ar atmosphere at 10 ° C. for 10 minutes to form an ohmic contact. Then, pure gold was deposited again on the AuBe alloy layer of this wafer by vacuum evaporation to a thickness of about 1 μm, and the p-GaAlAs current diffusion layer 3 formed on the p-GaP light-scattering layer was exposed by photolithography. The AuBe alloy layer and the pure gold layer are removed except for the portion. In this way, the p-side electrode 5 is formed on the glossy surface of the p-GaAlAs current diffusion layer 3. The reason why such a complicated process is adopted is that the electrode surface needs to have a gloss in order to detect the electrode during automatic wire bonding. Then, finally, it is diced at a predetermined pitch to be separated into individual pellets. In this way, a high-efficiency green LED having the p-side electrode 5 side as the light extraction side is completed. Since the light generated in the light emitting layer 2 is extracted to the outside from the surface on which the p-side electrode 5 is formed, this electrode becomes the light extraction-side electrode. That is, in this LED, the light generated in the active layer of the double hetero structure section goes to the p-side electrode 5 side, the substrate 1 side and the side surface. The light directed to the substrate 1 side is efficiently reflected by the light reflection layer 6 and directed to the light extraction side, and a part thereof is extracted from the light extraction surface, and the light directed to the p-type electrode 5 is also the same part. Are taken out from the light extraction surface. At this time, since the light extraction surface of the device is a light scattering layer, the light extraction efficiency is improved by about 2 times as compared with the conventional case where the light is extracted from the glossy surface of the current diffusion layer. To be realized. As described above, according to the embodiment, a high-brightness LED that emits light in the green region using a high-quality and inexpensive GaAs substrate can be manufactured without using a special substrate. Low cost green L
It can be said that mass production of EDs makes a great contribution to the information industry such as displays and optical communications.

【0014】ここで用いた光散乱層としてはGaPに限
定されることではなく、これと接して形成される電流拡
散層の材料の格子定数と異なった格子定数をもち、か
つ、発光色よりエネルギーの高いバンドギャップをもつ
ものなら光散乱層とすることができる。すなわち、格子
定数が0.3%以上異なる材料を発光素子の半導体層上
に0.5μm以上堆積させれば本発明の特徴である光散
乱層を形成することができる。もともと、各半導体層を
結晶性よく成長させなければ結晶面が荒れてしまい特性
が劣化するので、隣接する2つの半導体層は、出来るだ
け結晶の格子定数を合わせるようにしていた。しかし、
ここでは、逆に格子定数をずらすことに特徴があり、こ
のようにすることにより、半導体層の表面を粗面化す
る。InGaAlP系LEDの場合は、前記GaPの他
にZnSe、ZnSもしくはZnSe−ZnSなどの材
料が使われる。この実施例において、GaAlAs電流
拡散層の格子定数は、InGaAlP発光層の格子定数
と約0.13%以下しか相違しないため、GaAlAs
電流拡散層の表面は鏡面であるが、その上に成長するG
aPの格子定数は、約3.5%GaAlAsとは異なる
のでGaP光散乱層の表面に凹凸が形成される。したが
って、GaP結晶は、光を効果的に散乱させることがで
きる。ここで半導体結晶の格子定数をあげる。GaP
は、5.4512オングストローム(以下、Aと略記す
る)、GaAsは、5.6533A、Ga0. 3 Al0.7
Asは、5.6588A、Ga0.2 Al0.8 Asは、
5.6595Aであり、In0.5 (Ga1-x Alx
0.5 Pは、GaAsの格子定数とほぼ同じである。な
お、実施例では緑色LEDについて説明したが、InG
aAlP活性層の組成を適宜変えることにより、容易に
黄色、橙色、赤色、赤外LED等にも適用可能になる。
The light scattering layer used here is not limited to GaP, has a lattice constant different from the lattice constant of the material of the current diffusion layer formed in contact therewith, and has an energy rather than an emission color. A light-scattering layer can be used as long as it has a high band gap. That is, by depositing materials having a lattice constant different by 0.3% or more on the semiconductor layer of the light emitting element by 0.5 μm or more, the light scattering layer, which is a feature of the present invention, can be formed. Originally, unless the respective semiconductor layers were grown with good crystallinity, the crystal plane was roughened and the characteristics were deteriorated. Therefore, the adjacent two semiconductor layers were made to have the crystal lattice constants matched as much as possible. But,
Here, conversely, the feature is that the lattice constant is shifted, and by doing so, the surface of the semiconductor layer is roughened. In the case of the InGaAlP-based LED, a material such as ZnSe, ZnS or ZnSe-ZnS is used in addition to GaP. In this example, the lattice constant of the GaAlAs current spreading layer differs from that of the InGaAlP light emitting layer by only about 0.13% or less, so that the GaAlAs
The surface of the current diffusion layer is a mirror surface, but G which grows on it
Since the lattice constant of aP is different from about 3.5% GaAlAs, irregularities are formed on the surface of the GaP light scattering layer. Therefore, the GaP crystal can effectively scatter light. Here, the lattice constant of the semiconductor crystal is given. GaP
Is 5.4512 angstrom (hereinafter, abbreviated as A), GaAs is, 5.6533A, Ga 0. 3 Al 0.7
As is 5.6588A, Ga 0.2 Al 0.8 As is
5.6595 A and In 0.5 (Ga 1-x Al x ).
0.5 P is almost the same as the lattice constant of GaAs. Although the green LED has been described in the embodiment, InG
By appropriately changing the composition of the aAlP active layer, it can be easily applied to yellow, orange, red, infrared LEDs and the like.

【0015】つぎに、図2を参照して第2の実施例を説
明する。不純物濃度が3×1018/cm3 程度のn−G
aAs半導体基板1上に厚さ1μm、不純物濃度5×1
17/cm3 のn−In0.5 (Ga1-x Alx 0.5
クラッド層21、厚さ0.6μmのアンド−プIn0.5
(Ga1-y Aly 0.5 P活性層20、厚さ1μm、不
純物濃度5×1017/cm3 のp−In0.5 (Ga1-z
Alz 0.5 Pクラッド層22、さらに、厚さ7μm、
不純物濃度1×1018/cm3 のp−Ga0.3 Al0.7
As電流拡散層3を順次MOVPE法などで成長させ
る。つぎに半導体基板1の他の面にAu−Geなどのn
側電極4をオ−ミックコンタクトさせる。つぎに、この
電流拡散層3の上にZnをド−プした不純物濃度が5×
1017/cm3 程度のp−GaP光散乱層10を1μm
程度成長させる。このp−GaPの格子定数は、この電
流拡散層のp−GaAlAsの格子定数と一致しないた
めにp−GaPは、格子不整合による不完全成長とな
り、その成長面は、粗面となって、光散乱層10が形成
される。ついで、光散乱層10は、部分的にエッチング
除去して、電流拡散層3の表面を一部露出させる。そし
て、この電流拡散層3の露出面にAuBe合金層を蒸着
してから純金を1μm程度堆積させて、光取出し側電極
(p側電極)5を形成する。勿論、この光取出し側電極
5は、直接光散乱層10の上に形成することもできる。
Next, a second embodiment will be described with reference to FIG. N-G with an impurity concentration of about 3 × 10 18 / cm 3
1 μm thick on aAs semiconductor substrate 1, impurity concentration 5 × 1
0 17 / cm 3 n-In 0.5 (Ga 1-x Al x ) 0.5 P
Clad layer 21, 0.6 μm thick And-In In 0.5
(Ga 1-y Al y) 0.5 P active layer 20, a thickness of 1 [mu] m, the impurity concentration of 5 × 10 17 / cm 3 of p-In 0.5 (Ga 1- z
Al z ) 0.5 P clad layer 22, further having a thickness of 7 μm,
Impurity concentration 1 × 10 18 / cm 3 of p-Ga 0.3 Al 0.7
The As current diffusion layer 3 is sequentially grown by the MOVPE method or the like. Next, on the other surface of the semiconductor substrate 1, n such as Au-Ge is formed.
The side electrode 4 is brought into ohmic contact. Next, the impurity concentration of Zn doped on the current diffusion layer 3 is 5 ×.
The p-GaP light scattering layer 10 of about 10 17 / cm 3 is 1 μm thick.
Grow to a degree. Since the lattice constant of p-GaP does not match the lattice constant of p-GaAlAs of the current diffusion layer, p-GaP is incompletely grown due to lattice mismatch, and its growth surface becomes a rough surface. The light scattering layer 10 is formed. Then, the light scattering layer 10 is partially removed by etching to partially expose the surface of the current diffusion layer 3. Then, an AuBe alloy layer is vapor-deposited on the exposed surface of the current diffusion layer 3, and pure gold is deposited to a thickness of about 1 μm to form a light extraction side electrode (p side electrode) 5. Of course, the light extraction side electrode 5 can also be formed directly on the light scattering layer 10.

【0016】つぎに、図3を参照して第3の実施例を説
明する。ここで用いる半導体基板は発光層からの光に対
して透明であり、したがって、基板側には光反射層を設
けない。この半導体基板1には、例えば、n−GaPを
用い、活性層にはInGaAlPを使用する。このGa
P基板は、InGaAlP−LEDの発光色(緑色〜赤
色)に対して透明なため反射層を設ける必要はない。G
aP基板に、GaPを発光層とするLEDの場合には問
題は生じないが、GaP基板にInGaAlPを発光層
に用いると、発光層に格子不整合による格子欠陥が多発
するために発光効率が低下し、結果的に輝度の高いLE
Dが得られない。そこで、この実施例では、GaP基板
1とn−In0.5 (Ga1-x Alx 0.5 Pクラッド層
21、アンド−プIn0.5 (Ga1-y Aly 0.5 P活
性層20、p−In0.5 (Ga1- z Alz 0.5 Pクラ
ッド層22からなる発光層2との間に、In1-v Gav
P組成勾配層7(v=1→0.5)を成長させることに
より基板と発光層との間の格子定数の違いを吸収させる
方法が採られている。組成勾配層としては、In
1- v (Ga1-w Alw V P(v=1→0.5)を用い
ることもできる。この発光層2の上に、発光波長に対し
て透明なp−Ga0.2 Al0.8 As電流拡散層3を形成
する。この電流拡散層の上に形成される光取出し側電極
5およびp−GaP光散乱層10を前の第2の実施例と
同様の方法で形成する。基板側にも電極を形成するが、
基板底面での光の反射を効率良く行うために、基板側電
極4は、水玉模様の形状にする。電極での光吸収も無視
できないので、このような形状にして光の反射が基板底
面で均一に行われるようにする。また、水玉形状に限ら
ず、例えば、多角形など任意な形状にしても良い。
Next, a third embodiment will be described with reference to FIG. The semiconductor substrate used here is transparent to the light from the light emitting layer, and therefore, no light reflecting layer is provided on the substrate side. For example, n-GaP is used for the semiconductor substrate 1, and InGaAlP is used for the active layer. This Ga
Since the P substrate is transparent to the emission color (green to red) of InGaAlP-LED, it is not necessary to provide a reflective layer. G
No problem occurs in the case of an LED having GaP as a light emitting layer on an aP substrate. However, when InGaAlP is used as a light emitting layer on a GaP substrate, the light emitting efficiency is lowered due to frequent occurrence of lattice defects due to lattice mismatch in the light emitting layer. And, as a result, LE with high brightness
I can't get D. Therefore, in this embodiment, GaP substrate 1 and the n-In 0.5 (Ga 1- x Al x) 0.5 P cladding layer 21, and - flop In 0.5 (Ga 1-y Al y) 0.5 P active layer 20, p- In 0.5 (Ga 1- z Al z ) 0.5 P, the In 1-v Ga v
A method is adopted in which the difference in lattice constant between the substrate and the light emitting layer is absorbed by growing the P composition gradient layer 7 (v = 1 → 0.5). As the composition gradient layer, In
1- v (Ga 1-w Al w) V P (v = 1 → 0.5) can also be used. On this light emitting layer 2, a p-Ga 0.2 Al 0.8 As current diffusion layer 3 transparent to the emission wavelength is formed. The light extraction side electrode 5 and the p-GaP light scattering layer 10 formed on this current diffusion layer are formed by the same method as in the second embodiment. An electrode is also formed on the substrate side,
In order to efficiently reflect light on the bottom surface of the substrate, the substrate-side electrode 4 has a polka dot pattern. Since the light absorption at the electrodes cannot be ignored, the light is reflected uniformly on the bottom surface of the substrate in such a shape. Further, the shape is not limited to the polka dot shape, and may be an arbitrary shape such as a polygonal shape.

【0017】つぎに、図4を参照して第4の実施例を説
明する。この実施例では、光取出し側電極の直下に光反
射層を設けて、発光層からこの電極に向かった光を有効
に取出すようにしている。図のように、基板側電極4を
形成したn−GaAs基板1の上に第1の実施例におい
て使用したものと同じ第1の光反射層6を形成し、その
上にn−GaAlAsクラッド層21、アンド−プGa
AlAs活性層20、p−GaAlAsクラッド層22
からなる発光層2を形成する。ここで、クラッド層21
は、1μm程度、活性層20は、0.6μm程度の厚さ
であるが、光取出し電極が形成される側のクラッド層2
2は、これらより厚く10μm以上にする。このクラッ
ド層22は、GaAlAsからなるものであり、しか
も、厚く形成してあるので、これ自身が電流拡散層とし
ても用いられ、光取出し電極5電極からの電流をLED
チップ全面に均一に拡散させる事ができる。発光波長の
1/2程度の厚さのp−InAlPとInGaAlPと
が交互に積層された多層構造の第2の光反射層8が、こ
のクラッド層22の上に成長形成される。そして、その
上に電極のオ−ミック性を容易にするためのp−GaA
sコンタクト層9を介して、第1の実施例と同じ材料の
光取出し電極5を設け、このクラッド層22の露出して
いる部分に、p−GaP光散乱層10を格子の不整合を
利用して形成する。このチップに形成される各素子の大
きさの一例は、0.3mm角のものがあり、その時の光
取出し電極の半径は、例えば、0.14mm程度であ
る。この実施例では、赤色もしくは赤外線LEDが形成
される。
Next, a fourth embodiment will be described with reference to FIG. In this embodiment, a light-reflecting layer is provided immediately below the light-extraction-side electrode so that the light emitted from the light-emitting layer toward this electrode is effectively extracted. As shown in the figure, the same first light reflection layer 6 as that used in the first embodiment is formed on the n-GaAs substrate 1 on which the substrate side electrode 4 is formed, and the n-GaAlAs clad layer is formed thereon. 21, Ando Ga
AlAs active layer 20, p-GaAlAs clad layer 22
The light emitting layer 2 is formed. Here, the clad layer 21
Is about 1 μm and the active layer 20 is about 0.6 μm in thickness, but the cladding layer 2 on the side where the light extraction electrode is formed is
2 is 10 μm or more thicker than these. The clad layer 22 is made of GaAlAs and is thickly formed. Therefore, the clad layer 22 itself is also used as a current diffusion layer, and the current from the light extraction electrode 5 is supplied to the LED.
It can be spread evenly over the entire surface of the chip. A second light reflection layer 8 having a multilayer structure in which p-InAlP and InGaAlP having a thickness of about ½ of the emission wavelength are alternately laminated is grown and formed on the cladding layer 22. Then, p-GaA for facilitating the ohmic property of the electrode is formed thereon.
The light extraction electrode 5 made of the same material as that of the first embodiment is provided through the s contact layer 9, and the p-GaP light scattering layer 10 is provided on the exposed portion of the cladding layer 22 by utilizing the lattice mismatch. To form. An example of the size of each element formed on this chip is 0.3 mm square, and the radius of the light extraction electrode at that time is, for example, about 0.14 mm. In this embodiment, a red or infrared LED is formed.

【0018】以上、光取出し電極側に光散乱層を形成す
るに際して、半導体層間の格子の不整合を利用している
が、HClなどの酸を用いて表面を粗面化することも可
能である。HClの場合は、光散乱層はGaPが良く、
発光効率は30〜50%程向上する。また、GaAlA
sの光散乱層には、HNO3 を用いることができる。こ
の硝酸法によれば発光効率は、10〜20%程向上す
る。前述した例では、半導体基板には、n型を用いた
が、当然p型基板を用いることができる。
As described above, when the light scattering layer is formed on the light extraction electrode side, the lattice mismatch between the semiconductor layers is utilized, but the surface can be roughened by using an acid such as HCl. .. In the case of HCl, the light scattering layer is preferably GaP,
Luminous efficiency is improved by about 30 to 50%. In addition, GaAlA
HNO 3 can be used for the light scattering layer of s. According to this nitric acid method, the luminous efficiency is improved by about 10 to 20%. Although the n-type is used for the semiconductor substrate in the above-described example, a p-type substrate can be naturally used.

【0019】[0019]

【発明の効果】光取出し電極側(光取出し面)に形成し
た光散乱層の光散乱面により光は、外部に出やすくな
り、発光効率が著しく向上する。また、従来は、各半導
体層の格子定数をできる限り一致させていたのに、この
発明の光散乱層は、逆に他の半導体層とは格子定数を変
えるようにしたので、容易に半導体基板に形成されるよ
うになる。
The light-scattering surface of the light-scattering layer formed on the side of the light-extracting electrode (light-extracting surface) makes it easier for light to go out, and the luminous efficiency is significantly improved. Further, conventionally, the lattice constants of the respective semiconductor layers were made to match as much as possible, but the light scattering layer of the present invention, on the contrary, was designed to have a lattice constant different from that of the other semiconductor layers, so that the semiconductor substrate can be easily formed. Will be formed.

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

【図1】本発明の第1の実施例のLEDの素子構造を示
す断面図。
FIG. 1 is a sectional view showing an element structure of an LED according to a first embodiment of the present invention.

【図2】本発明の第2の実施例のLEDの素子構造を示
す断面図。
FIG. 2 is a sectional view showing an element structure of an LED according to a second embodiment of the present invention.

【図3】本発明の第3の実施例のLEDの素子構造を示
す断面図。
FIG. 3 is a sectional view showing an element structure of an LED according to a third embodiment of the present invention.

【図4】本発明の第4の実施例のLEDの素子構造を示
す断面図。
FIG. 4 is a sectional view showing an element structure of an LED according to a fourth embodiment of the present invention.

【図5】従来のLEDの素子構造を示す断面図。FIG. 5 is a sectional view showing a device structure of a conventional LED.

【符号の説明】[Explanation of symbols]

1 半導体基板 2 発光層 3 電流拡散層 4 基板側電極 5 光取出し側電極 6 光反射層 7 組成勾配層 8 光反射層 9 コンタクト層 10 光散乱層 1 semiconductor substrate 2 light emitting layer 3 current diffusion layer 4 substrate side electrode 5 light extraction side electrode 6 light reflecting layer 7 composition gradient layer 8 light reflecting layer 9 contact layer 10 light scattering layer

Claims (8)

【特許請求の範囲】[Claims] 【請求項1】 活性層を含む発光層と、 この発光層の上に形成され、光取出し面を有する光散乱
層と、 前記発光層もしくは前記光散乱層の上に形成された光取
出し側電極とを備えていることを特徴とする半導体発光
素子。
1. A light emitting layer including an active layer, a light scattering layer formed on the light emitting layer and having a light extraction surface, and a light extraction side electrode formed on the light emitting layer or the light scattering layer. And a semiconductor light emitting device.
【請求項2】 活性層を含む発光層と、 この発光層の上に形成された電流拡散層と、 この電流拡散層の上に形成され、光取出し面を有する光
散乱層と、 前記電流拡散層もしくは前記光散乱層の上に形成された
光取出し側電極とを備えていることを特徴とする半導体
発光素子。
2. A light emitting layer including an active layer, a current spreading layer formed on the light emitting layer, a light scattering layer formed on the current spreading layer and having a light extraction surface, and the current spreading layer. And a light extraction side electrode formed on the light scattering layer.
【請求項3】 前記発光層は、シングルヘテロ接合、ダ
ブルヘテロ接合もしくはホモ接合のいずれかを備えてい
ることを特徴とする請求項1又は請求項2に記載の半導
体発光素子。
3. The semiconductor light emitting device according to claim 1, wherein the light emitting layer has a single heterojunction, a double heterojunction, or a homojunction.
【請求項4】 前記発光層がInGaAlP系混晶半導
体を活性層として備えている半導体発光素子において、
前記光散乱層は、GaP、ZnS、ZnSeおよびZn
Se−ZnSから選ばれる材料を用いることを特徴とす
る請求項1又は請求項2に記載の半導体発光素子。
4. A semiconductor light emitting device, wherein the light emitting layer includes an InGaAlP-based mixed crystal semiconductor as an active layer,
The light scattering layer is made of GaP, ZnS, ZnSe and Zn.
The semiconductor light emitting device according to claim 1 or 2, wherein a material selected from Se-ZnS is used.
【請求項5】 前記光散乱層の厚さは、0.5μm以上
であり、その光散乱層の半導体結晶の格子定数は、その
底面と接する半導体結晶の格子定数とは0.3%以上異
なっていることを特徴とする請求項1又は請求項2に記
載の半導体発光素子。
5. The thickness of the light-scattering layer is 0.5 μm or more, and the lattice constant of the semiconductor crystal of the light-scattering layer is different from the lattice constant of the semiconductor crystal in contact with the bottom surface by 0.3% or more. The semiconductor light emitting element according to claim 1 or 2, wherein
【請求項6】 前記発光層の前記光散乱層が形成されて
いる面とは反対側の表面には、半導体基板が設けられ、
この半導体基板の前記発光層が形成されている面とは反
対側の表面には、基板側電極が設けられていることを特
徴とする請求項1又は請求項2に記載の半導体発光素
子。
6. A semiconductor substrate is provided on the surface of the light emitting layer opposite to the surface on which the light scattering layer is formed,
3. The semiconductor light emitting device according to claim 1, wherein a substrate-side electrode is provided on the surface of the semiconductor substrate opposite to the surface on which the light emitting layer is formed.
【請求項7】 前記半導体基板のバンドギャップが、前
記活性層のバンドギャップとほぼ同じか、あるいはそれ
より大きいバンドギャップを有するように半導体基板材
料を選ぶと共に、前記基板側電極は、水玉模様の形状を
有していることを特徴とする請求項6に記載の半導体発
光素子。
7. The semiconductor substrate material is selected so that the band gap of the semiconductor substrate is substantially equal to or larger than the band gap of the active layer, and the substrate-side electrode has a polka dot pattern. The semiconductor light emitting device according to claim 6, which has a shape.
【請求項8】 前記光取出し側電極の直下には光反射層
を形成したことを特徴とする請求項1又は請求項2に記
載の半導体発光素子。
8. The semiconductor light emitting device according to claim 1, wherein a light reflecting layer is formed immediately below the light extraction side electrode.
JP35164691A 1991-12-12 1991-12-12 Semiconductor light emitting device Expired - Lifetime JP3152708B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP35164691A JP3152708B2 (en) 1991-12-12 1991-12-12 Semiconductor light emitting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP35164691A JP3152708B2 (en) 1991-12-12 1991-12-12 Semiconductor light emitting device

Publications (2)

Publication Number Publication Date
JPH05167101A true JPH05167101A (en) 1993-07-02
JP3152708B2 JP3152708B2 (en) 2001-04-03

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