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JP2002222991A - Semiconductor light emitting device - Google Patents

Semiconductor light emitting device

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Publication number
JP2002222991A
JP2002222991A JP2001017486A JP2001017486A JP2002222991A JP 2002222991 A JP2002222991 A JP 2002222991A JP 2001017486 A JP2001017486 A JP 2001017486A JP 2001017486 A JP2001017486 A JP 2001017486A JP 2002222991 A JP2002222991 A JP 2002222991A
Authority
JP
Japan
Prior art keywords
semiconductor
zno
light
gan
emitting device
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
JP2001017486A
Other languages
Japanese (ja)
Other versions
JP3498140B2 (en
Inventor
Hiroya Iwata
拡也 岩田
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.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
National Institute of Advanced Industrial Science and Technology AIST
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Priority to JP2001017486A priority Critical patent/JP3498140B2/en
Publication of JP2002222991A publication Critical patent/JP2002222991A/en
Application granted granted Critical
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Expired - Lifetime legal-status Critical Current

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Abstract

(57)【要約】 【課題】 白色LEDは、白熱電球や蛍光灯と比較する
と、発光効率が良く、発熱が極めて少なく、低消費電力
なため、白熱電球や蛍光灯に変わる光源として注目さ
れ、携帯電話等のバックライトに既に使用されている
が、より広く普及させるには、さらに効率がよく、簡便
に大きな面積を作製できることが望まれている。 【解決手段】 そこで、ZnO系半導体とGaN系半導体とを
接合し、人間の視感度曲線に極めて近い発光特性にて発
光する白色LEDを、蛍光体を使わずに、簡易に製作す
ることとした。
(57) [Problem] A white LED is attracting attention as a light source replacing an incandescent lamp or a fluorescent lamp because it has better luminous efficiency, generates less heat, and consumes less power than an incandescent lamp or a fluorescent lamp. Although it is already used for backlights of mobile phones and the like, it is desired to be able to produce a large area more efficiently and simply in order to spread it more widely. In order to solve this problem, a ZnO-based semiconductor and a GaN-based semiconductor are joined together to easily produce a white LED that emits light with emission characteristics extremely close to a human visibility curve without using a phosphor. .

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本願発明は、人間の視感度曲
線に極めて近い発光特性で発光する白色半導体発光素子
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a white semiconductor light emitting device which emits light with light emission characteristics very close to a human visibility curve.

【0002】[0002]

【従来の技術】現在、半導体を用いた白色発光素子(L
ED)としては、2つの方式が存在する。これらを図2
及び図3を用いて説明する。最初に登場した白色LED
(図2参照)は、青色LEDの周りを黄色発光の蛍光体
で覆い、青色LEDから黄色発光の蛍光体を透過して直
接外部に届く青色の光及び青色LEDからの青色光を一
旦黄色発光の蛍光体で吸収し、そこから発せられる黄色
の光とを合成したものである。しかし、この方式は、青
色を一旦吸収して発光する分、効率が低下している。ま
た、作製プロセス上も通常のLEDより、蛍光体を介在
させる分だけ工程が多くなっている。次に、第2の方式
の白色LED(図3参照)は、青色ZnSe LEDのZnSe
基板からの蛍光を利用した白色LEDで、これも基板の
蛍光を利用する分効率が下がっている。
2. Description of the Related Art At present, a white light emitting device (L) using a semiconductor is known.
As ED), there are two methods. These are shown in FIG.
This will be described with reference to FIG. White LED first appeared
(Refer to FIG. 2) is that the blue LED is covered with a yellow-emitting phosphor, and the blue light transmitted from the blue LED through the yellow-emitting phosphor and directly reaches the outside and the blue light from the blue LED are once yellow-emitting. Is synthesized with the yellow light that is absorbed by the phosphor and emitted therefrom. However, in this method, the efficiency is reduced because the light is absorbed once by absorbing the blue light. In addition, in the manufacturing process, the number of steps is larger than that of a normal LED by the amount of the phosphor. Next, the white LED of the second type (see FIG. 3) is ZnSe of the blue ZnSe LED.
This is a white LED using the fluorescence from the substrate, and the efficiency of the white LED is also reduced by using the fluorescence from the substrate.

【0003】[0003]

【発明が解決しようとする課題】白色LEDは、白熱電
球や蛍光灯と比較すると、発光効率が良く、発熱が極め
て少なく、低消費電力なため、白熱電球や蛍光灯に変わ
る光源として注目され、携帯電話等のバックライトに既
に使用されているが、より広く普及させるには、さらに
効率がよく、簡便に大きな面積を作製できることが望ま
れている。
As compared with incandescent lamps and fluorescent lamps, white LEDs have attracted attention as light sources replacing incandescent lamps and fluorescent lamps, because they have better luminous efficiency, generate less heat, and consume less power. Although it is already used for backlights of mobile phones and the like, it is desired to be able to produce a large area more efficiently and simply in order to spread it more widely.

【0004】[0004]

【課題を解決するための手段】そこで、ZnO系半導体とG
aN系半導体との接合構造により、人間の視感度曲線に極
めて近い発光特性にて発光する白色LEDを、蛍光体を
使わずに、簡易に製作することとした。ここで、ZnO
系半導体とはZnO, ZnCdO, ZnMgO, ZnCdMgO, ZnOSe, ZnO
S等及びその組み合わせである、ZnCdMgOSSeである。ま
た、GaN系半導体とはGaN, GaInN, AlGaN 及び AlGaI
nNである。
[Means for solving the problem] Therefore, ZnO based semiconductors and G
A white LED that emits light with a light emission characteristic extremely close to a human luminosity curve due to a junction structure with an aN-based semiconductor is simply manufactured without using a phosphor. Here, ZnO
Based semiconductors are ZnO, ZnCdO, ZnMgO, ZnCdMgO, ZnOSe, ZnO
ZnCdMgOSSe which is S or the like and a combination thereof. GaN-based semiconductors include GaN, GaInN, AlGaN and AlGaI.
nN.

【0005】[0005]

【発明の原理及び作用】本願発明のLEDは、次のような
原理により発光する。従来の半導体発光素子は、全て同
じ半導体のp形半導体とn形半導体のpn接合により発光さ
せる仕組みであった。本願発明の発光原理は、異なる半
導体のp形半導体とn形半導体のpn接合により発光させる
新しい原理である。従来のダブルへテロ構造に用いられ
ているヘテロ構造は、屈折率や禁制帯幅が異なると言う
意味でのヘテロであるが、実際は同族半導体の混晶比を
変化したものにすぎなかった。従来の技術では、同族半
導体の混晶比を変化したものですら画期的であったが、
本発明のヘテロ構造は、完全に異族半導体間接合による
ヘテロ構造であり、従来、発光素子作製は困難とされて
きた。
The LED of the present invention emits light according to the following principle. Conventional semiconductor light-emitting devices all have a structure in which light is emitted by a pn junction of a p-type semiconductor and an n-type semiconductor, which are all the same semiconductor. The light emitting principle of the present invention is a new principle of emitting light by a pn junction of a p-type semiconductor and an n-type semiconductor of different semiconductors. The hetero structure used in the conventional double hetero structure is a hetero structure in which the refractive index and the forbidden band width are different from each other. However, in reality, it is only a structure in which the mixed crystal ratio of a homologous semiconductor is changed. In the conventional technology, even the one that changed the mixed crystal ratio of the family semiconductor was revolutionary,
The heterostructure of the present invention is a heterostructure completely formed by a junction between heterogeneous semiconductors, and it has been conventionally difficult to manufacture a light emitting device.

【0006】図1に、p形GaN半導体とn形ZnO半導体とと
を接合した発光デバイスの例を示す。なお、現状では、
ワイドバンドギャップ半導体で、実用に耐えるp形半導
体が実現されているのは、GaN半導体のみであること、
及び、異族半導体においてGaNとZnOほど格子定数が近接
している例は他にないので、p形GaN半導体とn形ZnO半導
体の組み合わせ以外のものにおいても白色半導体発光素
子となる可能性は低いと思われる。
FIG. 1 shows an example of a light emitting device in which a p-type GaN semiconductor and an n-type ZnO semiconductor are joined. In addition, at present,
Only GaN semiconductors have realized wide-bandgap semiconductors and practical p-type semiconductors.
And since there is no other example in which a lattice constant is as close as GaN and ZnO in a heterogeneous semiconductor, it is unlikely that the white semiconductor light emitting device will be a white semiconductor light emitting element even in a combination other than a combination of a p-type GaN semiconductor and an n-type ZnO semiconductor. Seem.

【0007】白色発光は、異種(ヘテロ)半導体接合
(あるいは、異族(ヘテロ)半導体接合と呼んだ方が、
正確かも知れない。)により発生する禁制帯中の準位を
利用する新しい原理を用いて発生させる。サブ準位が形
成される機構として、次のようなサブバンド形成が考え
られる。2-6族と3-5族のような族まで異なる半導体にお
いては、接合界面において結合する電子の過不足が生
じ、このため、同じ4配位でも2と6,3と5であるので、
余って結合しない電子(ダングリングボンド)、足りな
くて電子の穴が空く(ベーカンシー)ようなものを接合
界面に作って電子の過不足を補正しようとする。このよ
うなものが、サブバンドを形成する原因と考えられる。
また、寄与は少ないと思われるが、次のような効果も若
干含まれるものと考えられる。すなわち、バンドギャッ
プが同じであっても、つまり価電子帯と伝導帯の差が同
じでも、実際の価電子帯や伝導帯の位置が微妙に違って
いると考えられるので、接合界面にはポテンシャルの段
差(バンドオフセット)が生じ、それがサブバンドのよ
うに新たな発光再結合プロセスを形成して禁制帯幅中の
エネルギーでの発光を引き起こしているとも考えられ
る。
[0007] White light emission is called a heterogeneous (hetero) semiconductor junction (or a heterogeneous (hetero) semiconductor junction).
May be accurate. ) Is generated using a new principle that utilizes the levels in the forbidden band. The following sub-band formation is considered as a mechanism for forming a sub-level. In semiconductors different from the 2-6 group and the 3-5 group, there is an excess or deficiency in the number of electrons bonded at the junction interface.
An attempt is made to compensate for excess or deficiency of electrons by creating electrons (dangling bonds) that are not excessively bonded or holes that are not enough to open holes (vacancies) at the bonding interface. Such a phenomenon is considered to be a cause of forming a subband.
Although the contribution is considered to be small, it is considered that the following effects are also included. In other words, even if the band gap is the same, that is, even if the difference between the valence band and the conduction band is the same, it is considered that the actual positions of the valence band and the conduction band are slightly different. It is considered that a step (band offset) occurs, which forms a new light-emitting recombination process like a sub-band, and emits light with energy in the band gap.

【0008】このことにより、蛍光体や蛍光剤は不要と
なる。また、上述のように、異族半導体間接合界面のダ
ングリングボンドなどの形成は、その電子の過不足の補
い方が空間構造的に無数の組み合わせが可能で不特定多
数のサブ準位が形成されるために、上記界面準位は、連
続的に分布する。このため、人間の視感度曲線に極めて
近い白色発光スペクトルをもつ発光が可能となる。
[0008] This eliminates the need for a phosphor or a fluorescent agent. Further, as described above, formation of dangling bonds and the like at the junction interface between heterogeneous semiconductors can be performed in an infinite number of combinations in terms of spatial structure in order to compensate for excess or deficiency of electrons, and an unspecified number of sub-levels are formed. Therefore, the interface states are continuously distributed. For this reason, light emission having a white light emission spectrum that is very close to a human visibility curve can be obtained.

【0009】また、n形半導体部分にはZnO系半導体、p
形半導体部分にはCaN系半導体を用い、特に、n形半導体
部分にはエッチングが容易なZnO系半導体を用いること
により、素子への加工性が向上する特徴を持つ。
The n-type semiconductor portion includes a ZnO-based semiconductor and p-type semiconductor.
The use of a CaN-based semiconductor for the n-type semiconductor portion and, in particular, the use of a ZnO-based semiconductor that is easy to etch for the n-type semiconductor portion has the characteristic of improving the processability of the device.

【0010】[0010]

【実施例】本願発明の実施例を第1図を用いて説明す
る。第1図おいて、p形層として、サファイア(0001)面
基板上にMOCVD法を用いてMgをドーピングしてp形GaN層
を積層する。上記p-GaN層上に、n形ZnO層を作製して、p
n接合を形成する。ここで、族の異なるヘテロ接合作製
技術が必要となる。まず、超高真空中でp-GaN層を水素
プラズマ照射により、エッチングを施し、優れた界面形
成の下準備を行う。その水素プラズマ表面処理を経て、
ZnO層の成長を行う。実施例のデバイスにおいては、発
光層として、不純物を添加していないi-ZnO層を導入し
ている。その積層方法としては、MBE法を用いた。超高
純度Zn(純度7N)はKセルから、酸素源は高純度酸素
(純度6N)のプラズマを用いたRFラジカルセルから
それぞれ供給し、10nm程度の極薄いi-ZnO層を成長し
た。成長温度は、450〜600℃程度、成長中の成長室真空
度は10の-6乗Torr程度である。
An embodiment of the present invention will be described with reference to FIG. In FIG. 1, as a p-type layer, a p-type GaN layer is laminated on a sapphire (0001) plane substrate by doping Mg using a MOCVD method. On the p-GaN layer, an n-type ZnO layer was prepared,
Form an n-junction. Here, heterojunction fabrication techniques of different families are required. First, the p-GaN layer is etched by irradiation with hydrogen plasma in an ultra-high vacuum to prepare for excellent interface formation. After the hydrogen plasma surface treatment,
A ZnO layer is grown. In the device of the embodiment, an i-ZnO layer to which no impurity is added is introduced as the light emitting layer. As the laminating method, the MBE method was used. Ultra-high-purity Zn (purity 7N) was supplied from a K cell, and an oxygen source was supplied from an RF radical cell using plasma of high-purity oxygen (purity 6N), and an extremely thin i-ZnO layer of about 10 nm was grown. The growth temperature is about 450 to 600 ° C., and the degree of vacuum in the growth chamber during growth is about 10 −6 Torr.

【0011】最後に極薄いi-ZnO層上に、Gaを高濃度に
ドーピングしたn形ZnO層を成長させる。これも、i-ZnO
層に引き続きMBE法を用い、超高純度Zn(純度7N)はK
セルから、酸素源は高純度酸素(純度6N)のプラズマ
を用いたRFラジカルセルから、そして、ドーピング用
の超高純度Ga(純度7N)は、Kセルから供給した。成
長膜厚は、200nm程度。成長温度は、i-ZnO層より若干低
く350〜450℃程度、成長中の成長室真空度は10の-6乗To
rr程度である。
Finally, an n-type ZnO layer heavily doped with Ga is grown on the extremely thin i-ZnO layer. This is also i-ZnO
Using MBE method for the layer, ultra-high purity Zn (purity 7N)
From the cell, the oxygen source was supplied from an RF radical cell using a plasma of high purity oxygen (purity 6N), and the ultra high purity Ga (purity 7N) for doping was supplied from a K cell. The grown film thickness is about 200 nm. The growth temperature is slightly lower than the i-ZnO layer, about 350-450 ° C, and the growth chamber vacuum during growth is 10 −6
It is about rr.

【0012】電極構造を作製するために、i-ZnO層とn-Z
nO層を塩酸でエッチングする。本発明の発光素子製造過
程の利点のひとつとして、エッチングにはウェットエッ
チングが利用できることが挙げられる。塩酸系エッチャ
ントだと、ZnO系酸化物半導体は良好にエッチングさ
れ、GaN系窒化物半導体は全くエッチングされないとい
う、ほぼ完全な選択エッチング特性が存在する。これ
は、製造プロセスに大きなアドバンテージがあるのみな
らず、将来的にこの異族半導体間ヘテロ接合を利用した
半導体レーザー等構造の複雑なデバイスを作製する際、
選択エッチングが容易で、塩酸で易しくエッチングされ
るZnO系半導体部分にさまざまな構造を作り込むことが
可能となる。半導体レーザークラスの構造の複雑なデバ
イスになると、その構造の形体は現在でも無数に存在す
ることから、新たな短波長系レーザーダイオードの構造
操作の世界が開ける。現在の窒化物半導体レーザーの構
造は、そのエッチングのしにくさから、構造がおのずと
限られ、短波長レーザー構造の発展の妨げとなってい
る。そういった意味でも、本発明のZnO/GaN異族半導体
間ヘテロ接合は新たな可能性を開くものである。
In order to form an electrode structure, an i-ZnO layer and an nZ
Etch the nO layer with hydrochloric acid. One of the advantages of the light emitting element manufacturing process of the present invention is that wet etching can be used for etching. With a hydrochloric acid-based etchant, a ZnO-based oxide semiconductor is etched well, and a GaN-based nitride semiconductor is not etched at all. This not only has a great advantage in the manufacturing process, but also in the future, when fabricating a complex device such as a semiconductor laser using this heterojunction between heterogeneous semiconductors,
Selective etching is easy, and various structures can be formed in a ZnO-based semiconductor portion easily etched with hydrochloric acid. In the case of a device having a complex structure of a semiconductor laser class, since there are numerous forms of the structure even today, a new world of structural operation of a short wavelength laser diode is opened. The structure of the current nitride semiconductor laser is naturally limited due to its difficulty in etching, hindering the development of a short wavelength laser structure. In that sense, the heterojunction between ZnO / GaN heterogeneous semiconductors of the present invention opens up new possibilities.

【0013】最後に、n-ZnO層成長表面に負極電極をと
り、エッチングした後に露出するp-GaN層に正極(+)電
極をとる。負極電極金属にはインジウムを、正極電極に
は金を用いる。
Finally, a negative electrode is taken on the n-ZnO layer growth surface, and a positive (+) electrode is taken on the p-GaN layer exposed after etching. Indium is used for the negative electrode metal and gold is used for the positive electrode.

【0014】上記説明において、p形GaN層の下地の基
板は、必ずしも上述のサファイア(0001)面基板である必
要はなく、むしろ導電性のある基板としてSiC基板や、
最近開発されつつあるGaN基板の上や、同じサファイア
基板上でも、ELOG(epitaxial lateral pver growth)の
ような技術を応用したGaN層上に作製されたものの方
が、特性が向上する可能性がある。
In the above description, the substrate underlying the p-type GaN layer does not necessarily have to be the sapphire (0001) plane substrate described above, but rather a SiC substrate or a conductive substrate.
Even on a recently developed GaN substrate or the same sapphire substrate, the characteristics may be improved when fabricated on a GaN layer applying technology such as ELOG (epitaxial lateral pver growth) .

【0015】また、一部キャリア電子オーバーフロー防
止層として、p-GaN層上にp-AlGaN層を作製してもよい。
Further, a p-AlGaN layer may be formed on the p-GaN layer as a partial carrier electron overflow prevention layer.

【0016】実際発光デバイスを作製する場合には、量
子井戸層などより多くの層が必要となってくる。有力な
活性層と呼ばれる発光層の候補としてZnCdO混晶半導体
が挙げられる。この場合、Cdの含有量によって発光特性
を制御することが可能となる。
When actually manufacturing a light emitting device, more layers such as quantum well layers are required. A ZnCdO mixed crystal semiconductor is a candidate for a light-emitting layer called an active layer. In this case, the light emission characteristics can be controlled by the content of Cd.

【0017】本願発明の図1のLEDを実際に作製して電
流駆動させた時の発光特性を図4に示す。図4は、pn接合
に電流を流したときの発光強度特性と、電圧特性を表し
ている。異種半導体間ヘテロpn接合にもかかわらず、通
常半導体pn接合に見られる整流特性とLED特性が得られ
ている。発光しきい値電圧は約4Vで、注入電流密度は約
50A/cm2であった。
FIG. 4 shows light emission characteristics when the LED of FIG. 1 of the present invention is actually manufactured and driven by current. FIG. 4 shows a light emission intensity characteristic and a voltage characteristic when a current flows through the pn junction. Despite the hetero pn junction between different kinds of semiconductors, the rectification characteristics and LED characteristics normally found in semiconductor pn junctions are obtained. The emission threshold voltage is about 4V and the injection current density is about
It was 50 A / cm2.

【0018】本願発明の図1のLEDを実際に作製して発
光させた波長特性評価の結果を図5に示す。図5は、いか
なる波長の光がどういった強度で発光しているかを示し
ている。図中の背景の黒い部分は、人間の視覚の視感度
曲線である。従来の白色LEDは、青色発光と蛍光の両方
の発光を利用するので、図6のように2つのピークを持
ち、視感度曲線と重ならないが、本願発明のLEDでは、
連続的に分布するヘテロ接合の界面準位によりスムーズ
で連続的な曲線をもち視感度曲線に近い発光スペクトル
が得られる。
FIG. 5 shows the result of wavelength characteristic evaluation of the LED of FIG. 1 of the present invention actually produced and emitted. FIG. 5 shows what wavelength light is emitted at what intensity. The black part of the background in the figure is the visibility curve of human vision. The conventional white LED uses both blue light emission and fluorescent light emission, so it has two peaks as shown in FIG. 6 and does not overlap with the luminosity curve, but in the LED of the present invention,
An emission spectrum having a smooth and continuous curve and close to a luminosity curve can be obtained by the interface levels of the heterojunction distributed continuously.

【0019】本願発明の特徴であるn形半導体部分にはZ
nO系半導体、p形半導体部分にはGaN系半導体を用いた異
種半導体間ヘテロpn接合の発光素子の場合、界面準位を
制御することにより、図7のような違う発光特性をもっ
たLEDを作製することも可能である。実際に青緑色に発
光するLEDを作製して発光させた結果を図7に示す。この
ように、本願発明のLEDでは、紫外線領域から、可視光
全域、赤外波長領域にまで、分布するヘテロ接合の界面
準位を制御することにより発光色を変化させることが可
能である。
The n-type semiconductor portion, which is a feature of the present invention, has Z
In the case of a hetero-pn junction light-emitting device using a GaN-based semiconductor for the nO-based semiconductor and the p-type semiconductor, LEDs with different light-emitting characteristics as shown in Fig. 7 are controlled by controlling the interface state. It is also possible to produce. FIG. 7 shows the result of actually producing a blue-green LED and emitting light. As described above, in the LED of the present invention, the emission color can be changed by controlling the interface states of the heterojunction distributed from the ultraviolet region to the entire visible light region and the infrared wavelength region.

【0020】[0020]

【発明の効果】 本願発明の半導体発光素子は、人間の
視感度曲線と非常に近い連続的に分布する白色発光曲線
を有することから、白熱電球や蛍光灯にとって替わる新
しい時代の照明として普及する可能性がある。また、新
しい半導体ZnOを用いることにより、低消費電力の白色L
EDの普及を向上させることができ、環境対策、省エネル
ギーに貢献することができる。さらに、スピンコートや
スパッタ蒸着により作製できる可能性があるZnO系半導
体を用いることで、高い生産効率が得られることから、
大面積低コスト化が可能であり、白熱電球や蛍光灯にと
って替わる新しい時代の照明として普及する時の普及率
の高さも期待できる。
Since the semiconductor light emitting device of the present invention has a continuous white light emission curve very close to the human visibility curve, it can be widely used as a lighting in a new era replacing incandescent lamps and fluorescent lamps. There is. In addition, by using new semiconductor ZnO, low power consumption white L
The spread of ED can be improved, and it can contribute to environmental measures and energy saving. Furthermore, by using a ZnO-based semiconductor that can be produced by spin coating or sputter deposition, high production efficiency can be obtained.
A large area and low cost can be achieved, and a high penetration rate can be expected when it is widely used as lighting for a new era replacing incandescent lamps and fluorescent lamps.

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

【図1】本願発明に係るZnO/GaNヘテロ接合白色LED
の模式図。
FIG. 1 shows a ZnO / GaN heterojunction white LED according to the present invention.
FIG.

【図2】従来のInGaN系白色LEDの模式図。FIG. 2 is a schematic view of a conventional InGaN-based white LED.

【図3】従来のZnSe系白色LEDの模式図。FIG. 3 is a schematic view of a conventional ZnSe-based white LED.

【図4】本願発明に係る白色LEDの発光特性図。FIG. 4 is a light emission characteristic diagram of the white LED according to the present invention.

【図5】本願発明の白色LEDの発光スペクトル。FIG. 5 is an emission spectrum of the white LED of the present invention.

【図6】従来のInGaN系白色LEDの発光スペクトル。FIG. 6 is an emission spectrum of a conventional InGaN-based white LED.

【図7】本願発明に係る青緑色LEDの発光スペクト
ル。
FIG. 7 is an emission spectrum of the blue-green LED according to the present invention.

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 n形半導体部分にはZnO系半導体、p形半
導体部分にはGaN系半導体を用いることを特徴とする半
導体発光素子。
1. A semiconductor light emitting device wherein a ZnO-based semiconductor is used for an n-type semiconductor portion and a GaN-based semiconductor is used for a p-type semiconductor portion.
【請求項2】 請求項2記載の半導体発光素子におい
て、発光部分には、ZnO系半導体とGaN系半導体との接合
構造の界面準位を発光準位として利用することを特徴と
する半導体発光素子。
2. The semiconductor light-emitting device according to claim 2, wherein an interface state of a junction structure between the ZnO-based semiconductor and the GaN-based semiconductor is used as the light-emitting level in the light-emitting portion. .
【請求項3】 p形GaN系半導体上に、n形半導体として
のZnO系半導体を積層することにより作成した半導体発
光素子。
3. A semiconductor light emitting device formed by laminating a ZnO-based semiconductor as an n-type semiconductor on a p-type GaN-based semiconductor.
【請求項4】 p形GaN系半導体上に、スピンコート又は
スパッタ蒸着により、n形半導体としてのZnO系半導体を
積層することにより作成した半導体発光素子。
4. A semiconductor light emitting device formed by laminating a ZnO-based semiconductor as an n-type semiconductor on a p-type GaN-based semiconductor by spin coating or sputter deposition.
【請求項5】 請求項4記載の発光素子において、n形
半導体の一部をエッチングにより除去し、除去された部
分にp形の電極を形成した半導体発光素子。
5. The light-emitting device according to claim 4, wherein a part of the n-type semiconductor is removed by etching, and a p-type electrode is formed in the removed part.
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