JPH01205479A - End surface light emitting type semiconductor light emitting device - Google Patents

End surface light emitting type semiconductor light emitting device

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Publication number
JPH01205479A
JPH01205479A JP63030249A JP3024988A JPH01205479A JP H01205479 A JPH01205479 A JP H01205479A JP 63030249 A JP63030249 A JP 63030249A JP 3024988 A JP3024988 A JP 3024988A JP H01205479 A JPH01205479 A JP H01205479A
Authority
JP
Japan
Prior art keywords
light
light emitting
injection region
current injection
side surfaces
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
JP63030249A
Other languages
Japanese (ja)
Other versions
JP2655411B2 (en
Inventor
Hiroki Hirasawa
平沢 宏希
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 JP3024988A priority Critical patent/JP2655411B2/en
Publication of JPH01205479A publication Critical patent/JPH01205479A/en
Application granted granted Critical
Publication of JP2655411B2 publication Critical patent/JP2655411B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Led Devices (AREA)

Abstract

PURPOSE:To improve temperature characteristics of light output and light leading-out efficiency, by making both of the side surfaces of a current injection region not paral lel, and constituting their inclination angles with respect to the light emitting surface in the range of 90 deg. and more and less than 90 deg.+ a specified value. CONSTITUTION:The title semiconductor light emitting diode of end surface light emit ting type is provided with a stripe type current injection region 6. Both side surfaces of the current injection region 6 are not parallel, and the inclination angle theta(=90 deg.+x) with respect to a light emitting surface 12 is 95 deg.. As the distance from the light emit ting surface 12 increases, the interval between both side surfaces extends. As compared with the conventional current injection region, the angle is increased by 5 deg.. As a result, the lights generated in the two extended area parts are guided and enter the same light emitting surface 12 at an angle equal to or less than 95 deg., which are added each other and radiated outward. Since the area is large, the temperature dependency of the radiated light is little as compared with the conventional E/E LED. Further, the light emitting surface 12 and back surfaces 13, 14 do not become parallel on any surface. By this structure, the generation of stimulated emission light is restrained, and temperature dependency of light is decreased.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、端面発光型半導体発光装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to an edge-emitting semiconductor light-emitting device.

但し、半導体レーザは除く。However, semiconductor lasers are excluded.

〔従来の技術〕[Conventional technology]

従来の端面発光型半導体発光ダイオード(以下E/E 
LED)は、第3図(al 〜(CI K示すように、
その電流注入領域6は、長刀形のストライプ状であった
Conventional edge-emitting semiconductor light emitting diode (hereinafter referred to as E/E)
LED) as shown in Figure 3 (al ~ (CI K)
The current injection region 6 had a long sword-shaped stripe shape.

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

上述した従来のE/E LEDは、その放出光の成分の
甲に誘導放出光全面発光型半導体発光ダイオード(以下
S/E i、ED)よシ多く含んでいる。それは、S/
ELEDと比べ、E/E LEDは、その活性層中を光
が導波される距離が長いためである。
The conventional E/E LED described above contains more stimulated emission light than a full-emission type semiconductor light emitting diode (hereinafter referred to as S/E i, ED) in its emitted light component. That is S/
This is because, compared to ELEDs, E/E LEDs have a longer distance for light to be guided through their active layer.

一般に、誘導放出光は、自然放出光よシ、温度依存性が
強いため、誘導放出光をその放射光の成分に多く含むE
/E LEDは、S/E LED よシその放射光の温
度依存性が強くなる。
In general, stimulated emission light has a stronger temperature dependence than spontaneous emission light, so it contains a large amount of stimulated emission light as a component of the synchrotron radiation.
/E LED has stronger temperature dependence of emitted light than S/E LED.

まt、放射光の温度依存性を少くする方法として現在、 (1)  キャリアのライフタイムを短くする(発光部
にキャリアをドーピングするなどの手段による)。
Currently, methods for reducing the temperature dependence of emitted light include: (1) shortening the lifetime of carriers (by doping the light emitting part with carriers, etc.);

(2)電流密度を下げる(電流注入領域の面積音大さく
する)。
(2) Lower the current density (increase the area sound of the current injection region).

という2つの手段が用いられるが、いずれも、その光出
力は小さくなる。
These two methods are used, but in either case, the optical output is small.

つまυ、放射光の温度依存性を少くし、同時にその光I
J」刀を大きくするということができないという欠点が
ある。
Finally, υ reduces the temperature dependence of the synchrotron radiation and at the same time increases the
J" The drawback is that it is not possible to make the sword larger.

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

本発明の端面発光型半導体発光装置は、半導体基板上に
活性Nを屈折率の大きなクラッド層で挾んだ半導体ヘテ
ロ接合構造体を積層したペレットにストライプ状の電流
注入領域を設けてなる端面発光型半導体発光装置におい
て、前記電流注入領域の両側の側面が非平行で光出射面
となす角度θ〃よ、光の放射角α、クラッド層の屈折率
′f!:nとしであり、前記光出射面から離れるほど前
記両側の側面の出]隔が広がっているというものである
The edge-emitting semiconductor light-emitting device of the present invention is an edge-emitting semiconductor light-emitting device in which a striped current injection region is provided on a pellet in which a semiconductor heterojunction structure in which active N is sandwiched between cladding layers with a large refractive index is laminated on a semiconductor substrate. In a type semiconductor light emitting device, the angle θ between the non-parallel side surfaces of the current injection region and the light exit surface, the radiation angle α of the light, and the refractive index of the cladding layer 'f! :n, and the distance between the side surfaces on both sides increases as the distance from the light exit surface increases.

〔実施例〕〔Example〕

次に、本発明の実施例について図面を参照して説明フ゛
る。
Next, embodiments of the present invention will be described with reference to the drawings.

第1図は本発明の第1の実施例を示すペレットの上面図
である。なお、電流注入領域の形状以外は第3図(al
〜(C)に示した従来例と同じである。
FIG. 1 is a top view of a pellet showing a first embodiment of the present invention. Note that the shapes other than the current injection region are as shown in FIG. 3 (al.
This is the same as the conventional example shown in ~(C).

この実施例は、n型1nP基板1上にp+型In−〇a
AsP活性層3((λg=1.3μm)?、7屈折率軟
きなクラッドN(n型J:nP/i2.4)  で挾ん
だ半導体ヘテロ接合構造体を積層したペレットにストラ
イプ状の電流注入領域6を設けてなる端面発光型半導体
発光ダイオードにおいて、電流注入領域6の両側の側面
が非平行で光出射面12となす角度θ(=90°+X)
が95°であり、光出射面12から・離れるほど両側の
側面の間隔が広がっているというものである。
In this embodiment, a p+ type In-○a is formed on an n-type 1nP substrate 1.
AsP active layer 3 ((λg = 1.3 μm)?, 7 A stripe-like structure is formed on a stacked pellet of a semiconductor heterojunction structure sandwiched between soft cladding N (n-type J: nP/i2.4) with a soft refractive index. In an edge-emitting semiconductor light emitting diode provided with a current injection region 6, the angle θ (=90°+X) that the side surfaces on both sides of the current injection region 6 are non-parallel and form with the light exit surface 12 is
is 95°, and the distance between the side surfaces on both sides increases as the distance from the light exit surface 12 increases.

なお、ペレットの大きさは300μmX200μmの長
刀形、電流注入領域の長さは165μm1活性層厚さは
0.1μmとする。一般にE/E LEDの光放射角は
片側約20°、InPの屈折率を3.5、空気のそれを
1とすると 1sin20°=3,5 s i n x 、  x=
5.5゜であるから、光出射面から、95.5°以下の
角度をもって、導波される光は、その光出射面から、外
部へ放射される事になる。
The size of the pellet is 300 μm x 200 μm long sword, the length of the current injection region is 165 μm, and the thickness of the active layer is 0.1 μm. In general, the light emission angle of an E/E LED is about 20° on one side, and if the refractive index of InP is 3.5 and that of air is 1, then 1 sin 20° = 3,5 sin x, x =
Since the angle is 5.5 degrees, light guided from the light exit surface at an angle of 95.5 degrees or less will be radiated to the outside from the light exit surface.

本実施例では、第1図でもわかる通多、そのなす角を9
5°とした。従来の電流注入領域より、その角度が5°
広がった事で、その広がった2つの面積部(図中2つの
斜線部)で発光し、導波された光は、同一の光出射面1
2に95°以下の角度をもって入射するため、この光出
射部で足し合わさって、外部へ放出される。しかも、従
来の電流注入領域よ勺、その面積は大きくなっているた
め、従来のE/E LED 、1: ICその放出光の
温度依存性は少ない。
In this example, the angle made by the tsuta shown in Fig. 1 is 9
It was set to 5°. The angle is 5° compared to the conventional current injection region.
Due to the expansion, light is emitted in the two expanded areas (two shaded areas in the figure), and the guided light is directed to the same light exit surface 1.
2 at an angle of 95° or less, they are added together at this light output section and emitted to the outside. Moreover, since the area of the current injection region is larger than that of the conventional E/E LED, the temperature dependence of the emitted light is small.

さらに、本発明では、電流注入領域で発光した光を効率
よく導波させるため、側面には反射率の高い金属(Au
)からなるp側電極8をxプベーション膜7の上に蒸着
させている。その上、光出射面12の後方の面は、従来
よシ、光出射面と平行な面になると、この面で反射され
た光が再び光出射面に向い、導波している甲で誘導放出
をおこすので、これを押えるため、斜めにエツチングす
るという技術があったが、本発明ではこれに加え、どの
同一平面上でも光出射部12と後方の面13゜14が平
行にならない構造にし、誘導放出光の発生を押え、光の
温度依存性を少なくしている。
Furthermore, in the present invention, in order to efficiently guide the light emitted from the current injection region, the side surface is made of a metal with high reflectance (Au).
) is deposited on the x-povation film 7. Moreover, when the rear surface of the light emitting surface 12 becomes a surface parallel to the light emitting surface as in the conventional case, the light reflected from this surface is directed back to the light emitting surface and is guided by the waveguide. In order to suppress this, there is a technique of etching diagonally, but in addition to this, the present invention has a structure in which the light emitting part 12 and the rear surface 13° 14 are not parallel even on the same plane. , suppresses the generation of stimulated emission light and reduces the temperature dependence of light.

第2図は、本発明の第2の実施例を示すペレットの上面
図である。本実施例もInP基板上に形成された長波長
帯E/E LEDである。その寸法は、電流注入領域の
長さが300μmの他は第1の実施例と同じである。ま
た、光出射面12と、その2つの側面は第1の実施例と
同じように95°の角度で接しさせ、その電流注入領域
6の面積を広げ、かつ、広がった部分で発光した光を同
一の光出射面12から放射できる。さらに、電流注入領
域6をペレット全縦断させ、第1の実施例よりもその電
流注入領域6の面8tk広げている。
FIG. 2 is a top view of a pellet showing a second embodiment of the present invention. This example is also a long wavelength band E/E LED formed on an InP substrate. Its dimensions are the same as in the first embodiment except that the length of the current injection region is 300 μm. In addition, the light emitting surface 12 and its two side surfaces are brought into contact with each other at an angle of 95° as in the first embodiment, and the area of the current injection region 6 is expanded, and the light emitted from the expanded portion is The light can be emitted from the same light exit surface 12. Furthermore, the current injection region 6 is made to extend across the entire length of the pellet, and the surface 8tk of the current injection region 6 is made wider than in the first embodiment.

これに加え、本実施例では、光出射面12の後方にも光
出射面15.16を設けた。しかし、ここから出射され
る光は、放射される光の発光領域が第1の実施例でも述
べたように、出射面の法線方向よりそれぞれ±5.5°
の領域(図中斜線部)に限られ、その光出力は、前方の
光出射面12よシも弱い。そのため、この光出射ffi
〕15,16から放射される光は、モニタ光として利用
することが出来る。
In addition to this, in this embodiment, light exit surfaces 15 and 16 were also provided behind the light exit surface 12. However, as described in the first embodiment, the light emitted from this area has a light emitting area of ±5.5 degrees from the normal direction of the light emitting surface.
The light output is limited to the area (shaded area in the figure), and the light output is weaker than that of the front light exit surface 12. Therefore, this light output ffi
] The light emitted from 15 and 16 can be used as monitor light.

次に、光出射面12の後方の面13.14は、第1の実
施例と同じように、光出射面12とどの平面をとっても
平行vCならないような構造にしている。
Next, the rear surfaces 13 and 14 of the light emitting surface 12 are structured so that no plane is parallel vC to the light emitting surface 12, as in the first embodiment.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、端面発光型半導体発光装
置の光出射面とその対面による光共振器構造を互いに平
行となる部分をなくし、かつ、その電流注入領域の面I
Rk広<シ、その放射光の温度依存性を少なくすると同
時に、光出射面の側面の2面を光の放射角より算出され
る全反射角以下の角度を持って接しさせ、従来の90”
 ’i持って接しさせる構造よシ、外部へ放射される発
光領域を最大限に太きくし、その光出力をも上げること
ができるという効果がある。
As explained above, the present invention eliminates the parallel parts of the optical resonator structure formed by the light emitting surface and the facing surface of the edge-emitting semiconductor light emitting device, and the surface I of the current injection region.
Rk wide < shi, while reducing the temperature dependence of the emitted light, the two sides of the light exit surface are brought into contact with an angle less than the total reflection angle calculated from the radiation angle of the light, and the conventional 90"
The structure in which the light is held and brought into contact has the effect of maximizing the thickness of the light emitting area emitted to the outside and increasing its light output.

なお、本発明は、実施例で示した電流注入領域の形状に
拘束されるものでなく、 (1)光出射面の対面が光出射面と平行な面を構成しな
い節 (2)光出射面の側面が該光出射面と90°以上、90
゜+Sin  ”(sinα/n)以下の角度で構成さ
れている事 の2点を満足する電流注入領域を持つことで、光出力、
光取シ出し効率を向上させ、光出力の温度特性を向上さ
せるものである。
It should be noted that the present invention is not limited to the shape of the current injection region shown in the embodiments, and includes (1) a clause in which the opposite side of the light exit surface does not constitute a plane parallel to the light exit surface; (2) a light exit surface; side surface is at an angle of 90° or more with the light emitting surface, 90°
The optical output,
This improves the light extraction efficiency and the temperature characteristics of light output.

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

第1図及び第2図はそれぞれ本発明の第1.第2の実施
例を示すペレットの上面図、第3図(a)。 (bi 、 (clはそれぞれ従来例を示すペレットの
上面図。 正面図、断面図である。 1・・・・・・n型InP基板、2・・・・・・n型I
nP層、 3・・・・・・p+型InGaAsP活性層
、4・・・・・・p型InPクラッド層、5・・・・・
・p型InGaAsPキャップ層、6・・・・・・電流
注入領域、7・・・・・・パッシベーション膜、8・・
・・・・piltl電極、9・・・・・・n側電極、1
0・・・・・・溝、11・・・・・・コンタクト窓、1
2・・・・・・光出射面、13゜14・・・・・・光出
射面の対面、15.16・・・・・・モニタ光出射面。 代理人 弁理士  内 原   音 第1図 第2図
FIGS. 1 and 2 respectively show the first embodiment of the present invention. FIG. 3(a) is a top view of a pellet showing the second example. (bi, (cl) are top views of pellets showing conventional examples. They are a front view and a cross-sectional view. 1... n-type InP substrate, 2... n-type I
nP layer, 3...p+ type InGaAsP active layer, 4...p type InP cladding layer, 5...
-p-type InGaAsP cap layer, 6... current injection region, 7... passivation film, 8...
...Piltl electrode, 9...N side electrode, 1
0...Groove, 11...Contact window, 1
2...Light exit surface, 13 degrees 14...Opposite side of light exit surface, 15.16...Monitor light exit surface. Agent Patent Attorney Oto Uchihara Figure 1 Figure 2

Claims (1)

【特許請求の範囲】  半導体基板上に活性層を屈折率の大きなクラッド層で
挾んだ半導体ヘテロ接合構造体を積層したペレットにス
トライプ状の電流注入領域を設けてなる端面発光型半導
体発光装置において、前記電流注入領域の両側の側面が
非平行で光出射面となす角度θが、光の放射角をα、ク
ラッド層の屈折率をnとして、 90゜<θ≦90゜+Sin^−^1(sinα/n)
であり、前記光出射面から離れるほど前記両側の側面の
間隔が広がっていることを特徴とする端面発光型半導体
発光装置。
[Claims] In an edge-emitting semiconductor light-emitting device in which a striped current injection region is provided in a pellet in which a semiconductor heterojunction structure in which an active layer is sandwiched between cladding layers with a large refractive index is laminated on a semiconductor substrate. , the angle θ between the nonparallel side surfaces of the current injection region and the light exit surface is 90°<θ≦90°+Sin^−^1, where α is the radiation angle of light and n is the refractive index of the cladding layer. (sin α/n)
An edge-emitting semiconductor light-emitting device characterized in that the distance between the side surfaces on both sides increases as the distance from the light exit surface increases.
JP3024988A 1988-02-10 1988-02-10 Edge-emitting semiconductor light emitting device Expired - Lifetime JP2655411B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3024988A JP2655411B2 (en) 1988-02-10 1988-02-10 Edge-emitting semiconductor light emitting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3024988A JP2655411B2 (en) 1988-02-10 1988-02-10 Edge-emitting semiconductor light emitting device

Publications (2)

Publication Number Publication Date
JPH01205479A true JPH01205479A (en) 1989-08-17
JP2655411B2 JP2655411B2 (en) 1997-09-17

Family

ID=12298435

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3024988A Expired - Lifetime JP2655411B2 (en) 1988-02-10 1988-02-10 Edge-emitting semiconductor light emitting device

Country Status (1)

Country Link
JP (1) JP2655411B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0902978A1 (en) * 1996-06-05 1999-03-24 Sarnoff Corporation Light emitting semiconductor device
JP2010192603A (en) * 2009-02-17 2010-09-02 Seiko Epson Corp Light-emitting device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50158223A (en) * 1973-11-12 1975-12-22

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50158223A (en) * 1973-11-12 1975-12-22

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0902978A1 (en) * 1996-06-05 1999-03-24 Sarnoff Corporation Light emitting semiconductor device
EP0902978A4 (en) * 1996-06-05 2000-02-23 Sarnoff Corp Light emitting semiconductor device
US6417524B1 (en) 1996-06-05 2002-07-09 Princeton Lightwave Inc. Light emitting semiconductor device
JP2010192603A (en) * 2009-02-17 2010-09-02 Seiko Epson Corp Light-emitting device

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Publication number Publication date
JP2655411B2 (en) 1997-09-17

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