JPH03127872A - Light emitting semiconductor device - Google Patents

Light emitting semiconductor device

Info

Publication number
JPH03127872A
JPH03127872A JP1266453A JP26645389A JPH03127872A JP H03127872 A JPH03127872 A JP H03127872A JP 1266453 A JP1266453 A JP 1266453A JP 26645389 A JP26645389 A JP 26645389A JP H03127872 A JPH03127872 A JP H03127872A
Authority
JP
Japan
Prior art keywords
light emitting
light
region
type
emitting 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
Application number
JP1266453A
Other languages
Japanese (ja)
Inventor
Kazuhiro Sawa
沢 和弘
Toshio Matsuda
俊夫 松田
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP1266453A priority Critical patent/JPH03127872A/en
Publication of JPH03127872A publication Critical patent/JPH03127872A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To increase the light emitting output while holding the directivity by a method wherein a curved surface is formed so that a light from a light emitting region may be reflected in the central direction on both side rear surfaces of a crystal restricting the light emitting region by constricting current in a partial region of a light emitting diode. CONSTITUTION:No electrode is formed beneath a light emitting region 4 at all while a spherical surface is formed on the rear surface of a crystal having no electrode at all. Accordingly, any downward emitted light will not be absorbed into an interface between an n-type Ga1-XAlxAs 1 and an (n) side electrode 9 at all to be reflected in the central direction of the light emitting region 4 from a spherical surface 10 having its center 12 at higher position than the region 4 further to be taken outside passing through a spherical lens 11. Through these procedures, the light emitting output can be increased while holding the directivity.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、発光半導体装置の構造に関するものである。[Detailed description of the invention] Industrial applications The present invention relates to the structure of a light emitting semiconductor device.

従来の技術 近年、発光半導体装置、たとえば、発光ダイオードはカ
メラの自動焦点あわせのための測距用光源として用いら
れている。これらの光源は遠くまで光が届くことが必要
である。このため発光ダイオードとしては、発光出力が
大きいことと同時に指向性に優れていることが求められ
る。自動焦点あわせ用の発光ダイオードとして発光領域
を制限し、かつ発光ダイオードチップ上に球レンズを搭
載して集光することにより指向性を良くしたものがある
2. Description of the Related Art In recent years, light-emitting semiconductor devices, such as light-emitting diodes, have been used as distance-measuring light sources for automatic focusing of cameras. These light sources need to be able to reach long distances. Therefore, light emitting diodes are required to have high light emission output and excellent directivity. Some light-emitting diodes for automatic focusing have a limited light-emitting area and have improved directivity by mounting a ball lens on the light-emitting diode chip to condense light.

以下に従来の発光ダイオードについて説明する。A conventional light emitting diode will be explained below.

第3図は従来の発光ダイオードの断面を示すものである
。第3図において、■はn形 Ga1−xAe xAs (x=0.4) 、2はn形
G a+−xA(l xA s (x=0.2) 、3
はp形GaAs発光層、4は発光領域、5はp形Ga+
−xACxAs (x=0.35) 、6はn形Ga+
−xA12xAs (x=0.17)、7はp形不純物
の拡散によりp形に転換した Gap−xAe、XAs (x−0,17)、8はp側
電極、9はn側電極、11は球レンズである。
FIG. 3 shows a cross section of a conventional light emitting diode. In Fig. 3, ■ is n-type Ga1-xAe xAs (x=0.4), 2 is n-type Ga1-xAe xA (l xA s (x=0.2), 3
is a p-type GaAs light-emitting layer, 4 is a light-emitting region, and 5 is a p-type Ga+
-xACxAs (x=0.35), 6 is n-type Ga+
-xA12xAs (x=0.17), 7 is Gap-xAe converted to p-type by diffusion of p-type impurity, XAs (x-0,17), 8 is p-side electrode, 9 is n-side electrode, 11 is It is a spherical lens.

発光ダイオードに流れる電流は、p側電極8からp形波
散層7を経てp形Ga+−xAe xAs (x=0.
35)5、p形GaAs発光層3、n形G a 1−X
A Q、 xA s 2 、1、n側電極9へと流れる
The current flowing through the light emitting diode passes from the p-side electrode 8 through the p-type wave dispersion layer 7 to p-type Ga+-xAe xAs (x=0.
35) 5, p-type GaAs light emitting layer 3, n-type Ga 1-X
A Q, xA s 2 , 1, flows to the n-side electrode 9.

p形Ga1−xA& x As (x=0.35)5に
入った電流は第2図の中で矢印で示すように拡がりなが
らp形GaAs発光層3へと流れるが、p形Ga1−x
Af! xAs (x−〇、35)5の拡がり抵抗のた
め、p形GaAs発光層3のうち電流が流れる領域は制
限され、この領域のみで発光する。
The current that entered the p-type Ga1-xA & x As (x=0.35)5 flows to the p-type GaAs light-emitting layer 3 while spreading as shown by the arrow in FIG.
Af! Due to the spreading resistance of xAs (x-〇, 35) 5, the region of the p-type GaAs light emitting layer 3 through which current flows is restricted, and light is emitted only in this region.

この発光領域4で発光した光を球レンズ11で集光して
、平行光線に近い光にすることにより指向性を上げてい
る。
The light emitted from the light emitting region 4 is condensed by a ball lens 11, and the directivity is improved by converting the light into nearly parallel light.

発明が解決しようとする課題 発光領域で発光した光は、上方だけでなく下方へも向か
う。従来の構成では下方へ向かった光は、n形GaI−
xAexAs(X−0,4)1とn側電極9との界面で
吸収されてしまい、発光した光が有効に発光ダイオード
の外に出てこないために、発光出力が小さいという欠点
があった。
Problems to be Solved by the Invention The light emitted from the light emitting region travels not only upward but also downward. In the conventional configuration, the light directed downward is n-type GaI-
Since the emitted light is absorbed at the interface between xAexAs(X-0,4)1 and the n-side electrode 9 and does not effectively exit the light emitting diode, there is a drawback that the emitted light output is small.

本発明は上記従来の課題を解決するもので、発光して下
方に向かった光を有効に外部に取り出し、指向性を保持
した状態で、発光出力を高めた発光ダイオードを提供す
ることを目的とする。
The present invention solves the above-mentioned conventional problems, and aims to provide a light emitting diode that effectively extracts the downwardly emitted light to the outside and increases the light emitting output while maintaining the directivity. do.

課題を解決するための手段 この目的を達成するために本発明の発光ダイオードは一
部の領域に電流を狭窄して発光領域を制限した結晶裏面
側に、前記発光領域からの光を中心方向へ反射するよう
な曲面をそなえた構成とした。
Means for Solving the Problems In order to achieve this object, the light emitting diode of the present invention constricts the current in a part of the region to limit the light emitting region on the back side of the crystal, and directs light from the light emitting region toward the center. The structure has a reflective curved surface.

作用 この構成により、発光して下方へ向かった光が曲面で発
光領域の中心方向へ反射することにより、下方へ向かっ
た光も有効に球レンズを通して取り出せ、指向性を保っ
たまま発光出力を高めることができる。
Effect: With this configuration, the light emitted and directed downward is reflected by the curved surface towards the center of the light emitting area, allowing the downward light to be effectively extracted through the ball lens, increasing the light emitting output while maintaining directivity. be able to.

実施例 以下本発明の一実施例について、図面を参照しながら説
明する。第1図は本発明の一実施例における発光ダイオ
ードの断面を示すものである。第1図において、主要部
は第2図の従来例と同しであるが、裏面側に球状の面1
0をそなえている点が異なる。
EXAMPLE Hereinafter, an example of the present invention will be described with reference to the drawings. FIG. 1 shows a cross section of a light emitting diode in one embodiment of the present invention. In Fig. 1, the main parts are the same as the conventional example shown in Fig. 2, but there is a spherical surface 1 on the back side.
The difference is that it has 0.

このような発光ダイオードは第1図を参照して説明する
と、以下のようにして作製される。まず、n形GaAs
基板(不図示)上に液相エピタキシャル成長性により、
n形G al−xAe xA 5(x=0.4)1を8
0μm、n形 Ga1−xA& x As (x=0.2) 2を15
μm。
Such a light emitting diode will be explained with reference to FIG. 1, and is manufactured as follows. First, n-type GaAs
By liquid phase epitaxial growth on a substrate (not shown),
n-type Gal-xAe xA 5 (x=0.4) 1 to 8
0 μm, n-type Ga1-xA & x As (x=0.2) 2 to 15
μm.

p形GaAs発光層3を1μm、p形 Ga+−xAe x A s (x=0.35)5を2
1t m 。
The p-type GaAs light emitting layer 3 is 1 μm thick, and the p-type Ga+−xAe x A s (x=0.35) 5 is 2 μm thick.
1tm.

n形Ga1−xAexAs(x=0.17>6を2μm
と順次成長する。次にn形Ga1−xAexAs(x=
0.17)6のうち直径180μmの領域を過酸化水素
とアンモニアの混合液でエツチング除去し、n形Ga1
−xAe、As (x=0.17)6の表面および段差
部にp形不純物を拡散することにより1μmの深さのp
形に転換したGa1−xAexAs (x=0.17)
7を形成する。
n-type Ga1-xAexAs (x=0.17>6 2μm
and grow sequentially. Next, n-type Ga1-xAexAs (x=
0.17) A region with a diameter of 180 μm in 6 was removed by etching with a mixture of hydrogen peroxide and ammonia, and n-type Ga1
-xAe, As (x = 0.17) By diffusing p-type impurities on the surface and step part of 6, a p
Ga1-xAexAs (x=0.17)
form 7.

そしてp形に転換したG a 1−xA il! XA
 5(x=0.17)7上にAeを蒸着しn側電極8と
する。ついで前記n形GaAs基板(不図示)を過酸化
水素とアンモニアの混合液でエツチング除去し、n形G
aI−xAex As (x=0.4)1の裏面にA 
u / G e合金を蒸着し、フォトリソグラフィ法に
より、表面の直径180μmの段差部とは同心円状に、
直径2r・0μmの部分でA u / G e合金を除
去し、この部分に窓のあいた形状のn側電極9を形成す
る。そして直径200μmのn形GaI−xAex A
s (x=0.4)1の裏面部分を、硫酸、過酸化水素
と水の混合液でエツチングする。この時、円の周辺部は
エツチング速度が速いのに対し中心部は遅いためにエツ
チング部分は第1図に示すような球状の面10となる。
Then, G a 1-xA il! converted to p-type! XA
5 (x=0.17) 7 to form an n-side electrode 8. Next, the n-type GaAs substrate (not shown) is removed by etching with a mixture of hydrogen peroxide and ammonia, and the n-type GaAs substrate (not shown) is removed by etching with a mixture of hydrogen peroxide and ammonia.
aI-xAex As (x=0.4) A on the back side of 1
U/G e alloy was deposited and photolithography was used to form a concentric circle with a stepped portion with a diameter of 180 μm on the surface.
The A u/G e alloy is removed from a portion having a diameter of 2r.0 μm, and an n-side electrode 9 having a window shape is formed in this portion. and n-type GaI-xAex A with a diameter of 200 μm.
Etch the back surface of s (x=0.4)1 with a mixture of sulfuric acid, hydrogen peroxide, and water. At this time, since the etching speed is fast at the periphery of the circle but slow at the center, the etched portion becomes a spherical surface 10 as shown in FIG.

最後に、表面の直径180μmの段差部に球レンズ11
をエポキシ系の樹脂を用いて接着することにより発光ダ
イオードが作製される。
Finally, a ball lens 11 is placed on the stepped portion of the surface with a diameter of 180 μm.
A light emitting diode is produced by bonding the two using an epoxy resin.

電流は、p形に転換したGa1−xAexAs(x−0
,17)7の段差部を経てp形Ga+−xAe x A
s (x=0.3)5の中を拡がりながらp形GaAs
発光層3へと流れるために、発光領域4は表面の直径1
80μmの段差部とは同心円となる。裏面側の球状の面
10も表面の段差部とは同心円となる領域に形成してい
るため、発光領域4に対しても同心円状の領域となり、
球状の面10は同心円の中心軸上に中心をもつような球
の面となる。また、エツチング量を適当にすることによ
り、球の中心が発光領域付近もしくは発光領域よりも上
方の光軸−Lになるようにすることができる。
The current is Ga1-xAexAs (x-0
, 17) p-type Ga+-xAe x A through the step part of 7
p-type GaAs expanding inside s (x=0.3)5
In order to flow into the luminescent layer 3, the luminescent region 4 has a surface diameter of 1
It forms a concentric circle with the step portion of 80 μm. Since the spherical surface 10 on the back side is also formed in an area that is concentric with the stepped portion on the front surface, it is also a concentric area with respect to the light emitting area 4.
The spherical surface 10 is a spherical surface having its center on the central axis of concentric circles. Furthermore, by selecting an appropriate amount of etching, the center of the sphere can be positioned near the light emitting region or on the optical axis -L above the light emitting region.

このように、発光領域の真下には電極を形成せず、また
、この電極のない結晶裏面を球状の面を形成することに
より、発光して下方へ向かった先は、従来例のようにn
形G al−xA(! xA 5(x=0.4)1とn
側電極9との界面で吸収されることなく、球状の面10
で反射し、発光領域4の中心方向へ向かう。第2図は、
発光領域4よりも上に中心12をもつ球状の面10での
光の反射の例を示したものであり、図中の矢印で示すよ
うに発光領域4の中心方向に反射し、さらに、球レンズ
11を通って光は外へ取り出せる。
In this way, no electrode is formed directly below the light emitting region, and by forming a spherical surface on the back surface of the crystal without this electrode, the downward direction of the light emitted is n
Form Gal-xA (!xA 5(x=0.4)1 and n
The spherical surface 10 is not absorbed at the interface with the side electrode 9.
The light is reflected by the light emitting region 4 and goes toward the center of the light emitting region 4 . Figure 2 shows
This figure shows an example of reflection of light on a spherical surface 10 having a center 12 above the light emitting region 4. As shown by the arrow in the figure, light is reflected toward the center of the light emitting region 4, Light can be taken out through the lens 11.

以上のように本実施例によれば、発光領域に相対する裏
面領域に電極を形成せず、この領域には発光領域の中心
軸上の発光領域にほぼ等しいかもしくは発光領域よりも
上の光軸部に中心をもつような球状の面を形成すること
により、発光して下方に向かった光も有効に外部へ取り
出すことができる。
As described above, according to this embodiment, no electrode is formed on the back surface region facing the light emitting region, and this region has a light emitting region that is approximately equal to or above the light emitting region on the central axis of the light emitting region. By forming a spherical surface centered on the shaft, the emitted light directed downward can also be effectively extracted to the outside.

発明の効果 以上のように本発明によれば、発光領域に相対する裏面
領域には電極を形成せず、この領域が発光領域からの光
を発光領域の中心方向へ反射するような曲面とすること
により、発光して下方へ向かった光も有効に外部に取り
出すことができ、指向性を保持したまま、発光出力を高
めた発光半導体装置を実現できる。
Effects of the Invention As described above, according to the present invention, no electrode is formed on the back surface region facing the light emitting region, and this region has a curved surface that reflects light from the light emitting region toward the center of the light emitting region. As a result, the light that is emitted and directed downward can be effectively extracted to the outside, and a light emitting semiconductor device with increased light emission output while maintaining directivity can be realized.

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

第1図は本発明の一実施例発光ダイオードの断面図、第
2図は本発明の一実施例発光ダイオードの光の反射経路
概念図、第3図は従来の発光ダイオードの断面図である
。 1− =−n形GaI−xAexAs (x−〇、4)
、2−−−−−− n形Gap−xAi! x As 
(x=0.2) 、3・・・・・・p形GaAs発光層
、4・・・・・・発光領域、5・・・”・p形Gap−
xA+2 xAs (x=0.35)、6−・・・n形
Ga+−xA&x As (x=0.17)、7−・・
・p形不純物の拡散によりp形に転換したGa+−xA
e x As (x=0.17) 、8−p側電極、9
・・・・・・n側電極、10・・・・・・球状の面、1
1・・・・・・球レンズ。
FIG. 1 is a sectional view of a light emitting diode according to an embodiment of the present invention, FIG. 2 is a conceptual diagram of a light reflection path of a light emitting diode according to an embodiment of the present invention, and FIG. 3 is a sectional view of a conventional light emitting diode. 1- = -n-type GaI-xAexAs (x-〇, 4)
, 2------- n-type Gap-xAi! x As
(x=0.2), 3... p-type GaAs light emitting layer, 4... light emitting region, 5...'' p-type Gap-
xA+2 xAs (x=0.35), 6-... n-type Ga+-xA&x As (x=0.17), 7-...
・Ga+-xA converted to p-type by diffusion of p-type impurity
e x As (x=0.17), 8-p side electrode, 9
......n-side electrode, 10......spherical surface, 1
1... Ball lens.

Claims (2)

【特許請求の範囲】[Claims] (1)一部の領域に電流を狭窄して発光領域を制限した
結晶の裏面側に、前記発光領域からの光を中心方向へ反
射する曲面をそなえたことを特徴とする発光半導体装置
(1) A light-emitting semiconductor device characterized in that a curved surface that reflects light from the light-emitting region toward the center is provided on the back side of a crystal whose light-emitting region is restricted by confining a current in a part of the region.
(2)曲面が発光領域の中心位置もしくは光軸上に中心
をもつような球状の面であることを特徴とする請求項1
記載の発光半導体装置。
(2) Claim 1 characterized in that the curved surface is a spherical surface having its center at the center position of the light emitting region or on the optical axis.
The light emitting semiconductor device described.
JP1266453A 1989-10-13 1989-10-13 Light emitting semiconductor device Pending JPH03127872A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1266453A JPH03127872A (en) 1989-10-13 1989-10-13 Light emitting semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1266453A JPH03127872A (en) 1989-10-13 1989-10-13 Light emitting semiconductor device

Publications (1)

Publication Number Publication Date
JPH03127872A true JPH03127872A (en) 1991-05-30

Family

ID=17431148

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1266453A Pending JPH03127872A (en) 1989-10-13 1989-10-13 Light emitting semiconductor device

Country Status (1)

Country Link
JP (1) JPH03127872A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5989108A (en) * 1996-09-09 1999-11-23 Koyo Machine Industries Co., Ltd. Double side grinding apparatus for flat disklike work

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5989108A (en) * 1996-09-09 1999-11-23 Koyo Machine Industries Co., Ltd. Double side grinding apparatus for flat disklike work

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