JPS62172691A - Thin film el device - Google Patents

Thin film el device

Info

Publication number
JPS62172691A
JPS62172691A JP61013472A JP1347286A JPS62172691A JP S62172691 A JPS62172691 A JP S62172691A JP 61013472 A JP61013472 A JP 61013472A JP 1347286 A JP1347286 A JP 1347286A JP S62172691 A JPS62172691 A JP S62172691A
Authority
JP
Japan
Prior art keywords
dielectric layer
layer
transparent electrode
thin film
light
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
JP61013472A
Other languages
Japanese (ja)
Other versions
JPH0766856B2 (en
Inventor
渡部 武人
孝 楡
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.)
Komatsu Ltd
Original Assignee
Komatsu 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 Komatsu Ltd filed Critical Komatsu Ltd
Priority to JP61013472A priority Critical patent/JPH0766856B2/en
Priority to US06/947,782 priority patent/US4794302A/en
Priority to EP87100094A priority patent/EP0229627B1/en
Priority to DE3751206T priority patent/DE3751206T2/en
Priority to DE8787100094T priority patent/DE3777664D1/en
Priority to EP90125792A priority patent/EP0421494B1/en
Priority to FI870066A priority patent/FI83013C/en
Priority to KR1019870000081A priority patent/KR0132785B1/en
Publication of JPS62172691A publication Critical patent/JPS62172691A/en
Priority to US07/269,930 priority patent/US5006365A/en
Priority to US07/648,111 priority patent/US5133988A/en
Publication of JPH0766856B2 publication Critical patent/JPH0766856B2/en
Priority to KR1019950034085A priority patent/KR970000428B1/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本光明は、′a薄膜L素子に係り、特にil1度の向上
のための@造に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a thin film L element, and particularly to a structure for improving illumination degree.

[従来技術およびその問題点] 輝度の面で問題が多く照明用光源としての開発を断面せ
ざるを得なかった。硫化亜鉛(ZnS)系蛍光体粉末を
用いた分散型EL素子に代わって、薄膜蛍光体層を用い
た薄膜型EL素子が高輝度を得られることから近年注目
されてきている。
[Prior art and its problems] Development as a light source for illumination had to be abandoned due to many problems in terms of brightness. In place of dispersed EL devices using zinc sulfide (ZnS)-based phosphor powder, thin-film EL devices using thin-film phosphor layers have been attracting attention in recent years because they can provide high brightness.

薄膜EL素子は、発光層が透明な薄膜で構成されていて
粒状性がないため、外部から入射する光および発光層内
部で発光した光が散乱されてハレーションやにじみを生
じることがなく、鮮明でコントラストが高いことから、
車両への搭載用、コンピュータ端末等の表示装置あるい
は照明用として脚光を浴びている。
Thin-film EL elements have a light-emitting layer that is made of a transparent thin film and has no graininess, so light incident from the outside and light emitted inside the light-emitting layer are not scattered and cause halation or smearing, resulting in clear images. Due to its high contrast,
It is in the spotlight for use in vehicles, display devices for computer terminals, and lighting.

従来薄膜El素子の基本構造は、第3図に示す如く透光
性の基板1上に酸化錫(SnO2)層等からなる透明電
極2と第1の誘電体層3と、ZnS:Mn薄膜からなる
発光層4と、第2の誘電体層5と、アルミニウム(A」
)層等からなる背面電極6とが順次積層ゼしめられた2
申誘電体構造をなしている。
The basic structure of a conventional thin film El element is as shown in FIG. The light emitting layer 4, the second dielectric layer 5, and the aluminum (A)
) layers, etc., are sequentially laminated.
It has a dielectric structure.

そして、光光の過程は、以下に示づ如くである。The process of light is as shown below.

前記透明電極と前記背面電極との間に電圧を印加すると
、発光層内に誘起された電界によって界面単位にトラッ
プされていた電子が引き出されて加速され充分なエネル
ギーを得、この電子がMn(発光中心)の軌道電子に衝
突しこれを励起する。
When a voltage is applied between the transparent electrode and the back electrode, the electric field induced in the light-emitting layer pulls out the electrons trapped at each interface and accelerates them to obtain sufficient energy, and these electrons become Mn( It collides with the orbital electrons of the luminescent center) and excites them.

そしてこの励起された発光中心が基底状態に戻る際に発
光を行なう。
Then, when this excited luminescent center returns to the ground state, it emits light.

かかる@造の簿膜EL素子においては、発光層から発生
される光を効率良く外部に取り出すべく、第1の誘電体
層の屈折率と膜厚を制御する方法(特公昭58−556
35>等、さまざまな工夫がなされている。
In such a film EL device manufactured by @, a method of controlling the refractive index and film thickness of the first dielectric layer (Japanese Patent Publication No. 58-556
35>, etc., various efforts have been made.

ところで、このような簿膜EL素子の等価回路は第1の
誘電体層3、発光層4、第2の誘電体層5によって構成
される3つのコンデンサの直列接続体として表わずこと
かできる。従って、第1の誘電体層および第2の誘電体
層の比誘電率ε「1゜Cr2が、発光層の比誘電体率ε
1に比べて充分に大きい(εr1.εr2)+8.11
)とき、これらの電気容Fi Crl、 Cr2. C
jはCr1. Cr2> Cjとなるため、この素子へ
の外部からの印加電圧のほとんどが発光層にかかること
になり、低い駆動電圧で高輝度を得ることができる。
By the way, the equivalent circuit of such a film EL element can be expressed as a series connection of three capacitors constituted by the first dielectric layer 3, the light emitting layer 4, and the second dielectric layer 5. . Therefore, the dielectric constant ε of the first dielectric layer and the second dielectric layer is 1°Cr2, while the dielectric constant ε of the light emitting layer is
Sufficiently larger than 1 (εr1.εr2)+8.11
), these electric capacitances Fi Crl, Cr2. C
j is Cr1. Since Cr2>Cj, most of the externally applied voltage to this element is applied to the light emitting layer, and high brightness can be obtained with a low driving voltage.

駆IJI電圧の低下のためには、第1のy、電体層どし
て誘電率の大きなものを用いるのが好ましいが、誘電率
の大きなものを用いると、透明電極との界面での反射率
が大きくなり、発光層からの光を効率良く取り出すこと
ができないという矛盾があり、低い駆動電圧で高輝度を
(qることは困難であった。
In order to reduce the driving IJI voltage, it is preferable to use a material with a large dielectric constant as the first y, electric layer, etc. However, if a material with a large dielectric constant is used, reflections at the interface with the transparent electrode may occur. There is a contradiction in that the ratio becomes large and light cannot be extracted efficiently from the light emitting layer, and it is difficult to achieve high brightness with a low driving voltage.

〔発明の目的〕[Purpose of the invention]

本発明は、前記実情に鑑みてなされたもので、発光層か
らの光を効率良く取り出し、高輝度を得ることのできる
薄膜EL素子を提供することを目的とする。
The present invention has been made in view of the above-mentioned circumstances, and an object of the present invention is to provide a thin film EL element that can efficiently extract light from a light emitting layer and obtain high brightness.

〔問題点を解決するための手段) そこで本発明では、基板上に透明電極と、第1の誘電体
層と、発光層と、第2の誘電体層と、背面電極とを順次
積層せしめた薄膜EL素子において、透明電極と第1の
誘電体層との間に、両者の中間の屈折率を有する第3の
誘電体層を介在せしめるようにしている。
[Means for Solving the Problems] Therefore, in the present invention, a transparent electrode, a first dielectric layer, a light emitting layer, a second dielectric layer, and a back electrode are sequentially laminated on a substrate. In the thin film EL element, a third dielectric layer having a refractive index intermediate between the transparent electrode and the first dielectric layer is interposed between the transparent electrode and the first dielectric layer.

〔作 用〕[For production]

かかる構成によれば、第3の誘電体層を介在せしめるこ
とにより第1の誘電体層のもつ誘電率を低下せしめるこ
となく第1の誘電体層と透明電極との界面における屈折
率の差を緩和し、反射を低減することにより発光層から
の光を効率良くとり出すことができる。
According to this configuration, by interposing the third dielectric layer, the difference in refractive index at the interface between the first dielectric layer and the transparent electrode can be reduced without reducing the dielectric constant of the first dielectric layer. By relaxing and reducing reflection, light can be efficiently extracted from the light emitting layer.

例えば、いま透明電極の屈折率をno=2、第1の誘電
体層を屈折率n2=4とし、これらの間にこれらの中間
の屈折率n1=3を有する第3のF:、電体層を介在さ
せたとき、フレネル(Fresnel )の法則より、
透明電極と第3の誘電体層との間の=2% 第3の誘電体層と第1の誘電体層との間の反射−4% となって全体の反射率は6%となり、透過率は94%と
なる。
For example, let us assume that the refractive index of the transparent electrode is no=2, the first dielectric layer has a refractive index n2=4, and a third F:, an electric material having an intermediate refractive index n1=3 is formed between them. When a layer is interposed, according to Fresnel's law,
The reflection between the transparent electrode and the third dielectric layer = 2%, the reflection between the third dielectric layer and the first dielectric layer - 4%, and the total reflectance is 6%. The rate is 94%.

これに対し、第3の誘電体層を介在さゼなかったとき、
透明電極と第1の誘電体層との反射率は、か11% となり、透過率は89%となる。
On the other hand, when the third dielectric layer is not interposed,
The reflectance between the transparent electrode and the first dielectric layer is approximately 11%, and the transmittance is 89%.

これら透過率の比較からも第3の誘電体層を介在せしめ
ることにより、透過率が大幅に改善されていることがわ
かる。
A comparison of these transmittances also shows that the interposition of the third dielectric layer significantly improves the transmittance.

(実施例) 以下、本発明の実施例について図面を参照しつつ詳細に
説明する。
(Example) Hereinafter, an example of the present invention will be described in detail with reference to the drawings.

第1図は、本発明のnb膜EL素子を示す図である。FIG. 1 is a diagram showing an nb film EL device of the present invention.

この薄rf5EL素子はjνさ1 rtrmの透光性の
ガラス基板11上にPIA厚0.3.czynの酸化錫
(SnO2)層等からなる透明型#A12、膜厚0.1
μmの酸化イツ・トリウム(Y2O2)層からなる第3
の誘電体層13、膜厚0.4μmの五酸化タンクル(T
a205)層からなる第1の誘電体層14、膜厚O15
μmの硫化亜鉛(ZnS):マンガンMn層からなる発
光層15.11!、!厚0.5μmの五酸化タンタル(
Ta205)層からなる第2の誘電体層16、膜厚0.
5μmのアルミニウム;W膜からなる背面電極17とが
順次積層セしめられて構成されている。
This thin rf5EL element is mounted on a transparent glass substrate 11 with a length of 1 rtrm and a PIA thickness of 0.3. Transparent type #A12 consisting of czyn tin oxide (SnO2) layer, etc., film thickness 0.1
The third layer consists of μm thick thorium oxide (Y2O2) layer.
The dielectric layer 13 is made of tank pentoxide (T) with a film thickness of 0.4 μm.
a205) first dielectric layer 14, film thickness O15
μm zinc sulfide (ZnS): Luminescent layer consisting of a manganese Mn layer 15.11! ,! Tantalum pentoxide with a thickness of 0.5 μm (
The second dielectric layer 16 is made of a Ta205) layer with a film thickness of 0.
A back electrode 17 made of a 5 μm thick aluminum film and a W film are sequentially laminated and set.

この薄膜EL素子は、透明電極と背面電極との間に交’
a 電界を加えることによって駆動されるが、その電圧
−輝度特性曲線aを従来例の第3の誘電体層を有しない
@造の薄1!EL素子の電圧−輝度特性曲線すと共に第
2図に示す。これらの比較からも、本発明の薄膜EL素
子は、従来例の薄膜ELi子に比べて、大幅にig!!
度が向上していることがわかる。(ここでたて軸は輝度
、横軸は印加電圧(V)を示す、、) なお、実施例では第3の誘電体層を一層@造としたが、
多層構造とし、徐々に屈折率の変化するような構造とし
てもよい。
This thin film EL element has an intersection between a transparent electrode and a back electrode.
a It is driven by applying an electric field, but its voltage-brightness characteristic curve a is similar to that of the conventional example, which does not have the third dielectric layer. FIG. 2 shows the voltage-luminance characteristic curve of the EL element. From these comparisons, the thin film EL device of the present invention has significantly higher ig! than the conventional thin film EL device. !
It can be seen that the level has improved. (Here, the vertical axis shows the brightness, and the horizontal axis shows the applied voltage (V).) In the example, the third dielectric layer was made of a single layer, but
It may also be a multilayer structure in which the refractive index gradually changes.

また、各層の構成材料としては、実施例に限定されるこ
となく、適宜変更可能である。加えて、この薄膜EL素
子は、表示装置以外に照明用として、光記録媒体への信
号の書き込み、読み出し、消去用の光源としても使用可
能である。
Further, the constituent materials of each layer are not limited to the examples and can be changed as appropriate. In addition, in addition to display devices, this thin film EL element can also be used for illumination and as a light source for writing, reading, and erasing signals on optical recording media.

(効 果) 以上説明したきたように、本発明によれば、透明電極と
第1の誘電体層との間に、これらの中間の屈折率を有す
る第3の誘電体層を介在せしめるようにしているため、
発光層からの光を効率良く、外部に取り出すことができ
、高輝度のW膜EL素子を提供することが可能となる。
(Effects) As explained above, according to the present invention, a third dielectric layer having a refractive index intermediate between the transparent electrode and the first dielectric layer is interposed between the transparent electrode and the first dielectric layer. Because
Light from the light-emitting layer can be efficiently extracted to the outside, making it possible to provide a high-luminance W film EL element.

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

第1図は、本発明実施例の1WIIWEL素了を示す図
、第2図は、同簿膜EL素子と従来の薄膜EL素子との
輝度−電圧特性の比較図、第3図は、従来例の薄膜EL
素子を示す図である。 1・・・基板、2・・・透明電極、3・・・第1の誘電
体層、4・・・発光層、5・・・第2の誘電体層、6・
・・背面τ、極、11・・・ガラス基板、12・・・透
明電極、13・・・第3の誘電体層、14・・・第1の
誘電体層、15・・・発光層、16・・・第2の誘電体
層、17・・・背面電極。 (−一・1.ム、二°、1 電圧 (■) 第2図
FIG. 1 is a diagram showing the completion of 1WIIWEL according to an embodiment of the present invention, FIG. 2 is a comparison diagram of brightness-voltage characteristics between the same film EL element and a conventional thin film EL element, and FIG. 3 is a diagram of a conventional example. thin film EL
It is a figure showing an element. DESCRIPTION OF SYMBOLS 1... Substrate, 2... Transparent electrode, 3... First dielectric layer, 4... Light emitting layer, 5... Second dielectric layer, 6...
...Back surface τ, pole, 11...Glass substrate, 12...Transparent electrode, 13...Third dielectric layer, 14...First dielectric layer, 15...Light emitting layer, 16... Second dielectric layer, 17... Back electrode. (-1・1.mu, 2°, 1 voltage (■) Fig. 2

Claims (1)

【特許請求の範囲】  透明電極と発光層との間に第1の誘電体層を介在せし
めると共に、更に透明電極側に、 該第1の誘電体層と透明電極との間の中間の屈折率を有
する第2の誘電体層を介在せしめるようにしたことを特
徴とする薄膜EL素子。
[Claims] A first dielectric layer is interposed between the transparent electrode and the light-emitting layer, and a refractive index intermediate between the first dielectric layer and the transparent electrode is further provided on the transparent electrode side. 1. A thin film EL device characterized by interposing a second dielectric layer having:
JP61013472A 1986-01-08 1986-01-24 Thin film EL device Expired - Fee Related JPH0766856B2 (en)

Priority Applications (11)

Application Number Priority Date Filing Date Title
JP61013472A JPH0766856B2 (en) 1986-01-24 1986-01-24 Thin film EL device
US06/947,782 US4794302A (en) 1986-01-08 1986-12-30 Thin film el device and method of manufacturing the same
EP87100094A EP0229627B1 (en) 1986-01-08 1987-01-07 Thin film electroluminescent device and method of manufacturing the same
DE3751206T DE3751206T2 (en) 1986-01-08 1987-01-07 Thin film electroluminescent device and method of manufacturing the same.
DE8787100094T DE3777664D1 (en) 1986-01-08 1987-01-07 THICK LAYER ELECTROLUMINESCENT DEVICE AND METHOD FOR PRODUCING THE SAME.
EP90125792A EP0421494B1 (en) 1986-01-08 1987-01-07 A thin film electroluminescent (EL) device and method of manufacturing the same
KR1019870000081A KR0132785B1 (en) 1986-01-08 1987-01-08 Thin film el device and method of manufacturing the same
FI870066A FI83013C (en) 1986-01-08 1987-01-08 Thin film type electroluminescence device and method of counting its front
US07/269,930 US5006365A (en) 1986-01-08 1988-10-28 Method of manufacturing a thin film EL device by multisource deposition method
US07/648,111 US5133988A (en) 1986-01-08 1991-01-31 Method of manufacturing thin film el device
KR1019950034085A KR970000428B1 (en) 1986-01-08 1995-10-02 Thin film el device and method for manufacturing the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61013472A JPH0766856B2 (en) 1986-01-24 1986-01-24 Thin film EL device

Publications (2)

Publication Number Publication Date
JPS62172691A true JPS62172691A (en) 1987-07-29
JPH0766856B2 JPH0766856B2 (en) 1995-07-19

Family

ID=11834073

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61013472A Expired - Fee Related JPH0766856B2 (en) 1986-01-08 1986-01-24 Thin film EL device

Country Status (1)

Country Link
JP (1) JPH0766856B2 (en)

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