JPH02256192A - Thin film el element and manufacture thereof - Google Patents

Thin film el element and manufacture thereof

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Publication number
JPH02256192A
JPH02256192A JP1276718A JP27671889A JPH02256192A JP H02256192 A JPH02256192 A JP H02256192A JP 1276718 A JP1276718 A JP 1276718A JP 27671889 A JP27671889 A JP 27671889A JP H02256192 A JPH02256192 A JP H02256192A
Authority
JP
Japan
Prior art keywords
electrode
emitting layer
thin film
light emitting
electrodes
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
JP1276718A
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Japanese (ja)
Other versions
JP2838111B2 (en
Inventor
Hideaki Yamagishi
秀章 山岸
Seiji Haneda
聖治 羽田
Koichi Ishii
石井 浩市
Hidetoshi Uehara
上原 秀俊
Hitoshi Hara
仁 原
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.)
Yokogawa Electric Corp
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Yokogawa Electric Corp
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Priority to JP1276718A priority Critical patent/JP2838111B2/en
Publication of JPH02256192A publication Critical patent/JPH02256192A/en
Application granted granted Critical
Publication of JP2838111B2 publication Critical patent/JP2838111B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To melt one electrode and stop the melting of a luminous layer when the luminous layer and an insulating layer have a defect and the portion is melted by the voltage application by using a member with the melting point lower than that of the portion consisting of the luminous layer and the insulating layer for one electrode. CONSTITUTION:The first electrode 2 is made of an oxide (ITO) of indium and tin, the second electrode 6 is made of Al, and the voltage is applied and gradually increased. When a defect exists on a film, the Al electrode, insulating layers 3 and 5, and a luminous layer 4 are broken by the voltage lower than the insulation withstanding value of an insulating material into the conductive state and locally melted, and Al (portion shown by A) with the melting point lower than that of the insulating layers 3 and 5 and the ITO are first melted and evaporated. The insulating layers 3 and 5 are left and Al (portion shown by A) is melted on them. The insulation state of the portion is immediately recovered. The melting of the insulating layers 3 and 5 is not continued, and it is locally stopped and is not spread over the whole picture elements.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明は、交流電界の印加により発光する薄膜エレクト
ロルミネッセンス(EL)素子に関し。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a thin film electroluminescent (EL) device that emits light upon application of an alternating current electric field.

電極材料の改良により素子の絶縁耐圧および歩留りの向
上をはかった薄膜EL素子に関するものである。
The present invention relates to a thin film EL device in which the dielectric breakdown voltage and yield of the device are improved by improving electrode materials.

〈従来の技術〉 第8図は発光層を挟んで形成した2重絶縁構造の薄膜E
 L素子の一例を示す断面図である。図において、1は
ガラス基板、2は酸化インジウム(In203)あるい
はインジウムと錫との酸化物(T i’ O)などから
なる透明な第1電極、3はS i 02やA l 20
3などからなる第1絶縁層である。上記ITOは透明度
、比抵抗、スペクトル吸収、パターン形成の容易さなど
他の材質に比較してずぐれているのでEL素子の電極と
して広く用いられている。4はMnあるいは希土類化合
物を添加したZnS発光層、5は第1絶縁層と同様の材
質からなる第2絶縁層、6はAIなどからなる第2電極
である。
<Prior art> Figure 8 shows a thin film E with a double insulation structure formed with a light-emitting layer sandwiched in between.
FIG. 3 is a cross-sectional view showing an example of an L element. In the figure, 1 is a glass substrate, 2 is a transparent first electrode made of indium oxide (In203) or an oxide of indium and tin (T i'O), and 3 is S i 02 or Al 20
The first insulating layer is made of 3 or the like. ITO is widely used as an electrode for EL devices because it is superior to other materials in terms of transparency, specific resistance, spectral absorption, and ease of pattern formation. 4 is a ZnS light emitting layer doped with Mn or a rare earth compound, 5 is a second insulating layer made of the same material as the first insulating layer, and 6 is a second electrode made of AI or the like.

上記構成のEL素子は第1電極2と第2電極6との間に
交流電源15により交流電界を印加すると、1〜2X1
0’V/cm程度の電界により発光する。
When an AC electric field is applied between the first electrode 2 and the second electrode 6 by the AC power source 15, the EL element with the above configuration is 1 to 2×1
Light is emitted by an electric field of about 0'V/cm.

〈発明が解決しようとする課題〉 近年航空機のフラットパネル等に用いるために第8図に
示す第2電極を第1電極と同様のI T’ 0からなる
透明電極で形成し、その上に更に異なる色の発光層を積
層した多色ELパネルを実現することが試みられている
。
<Problem to be solved by the invention> In recent years, for use in aircraft flat panels, the second electrode shown in FIG. 8 is formed of a transparent electrode made of I T' 0 similar to the first electrode, and Attempts have been made to realize a multicolor EL panel in which light emitting layers of different colors are laminated.

しかしながら1発光層を発光させるために電極に電圧を
印加すると、膜のピンホールやゴミ、欠陥等を中心に局
部的に絶縁破壊が発生し、その破壊がEL画素全体に波
及(伝搬型破壊と呼ばれる)して画素欠けを生し、パネ
ルの表示品質を著しく損うという問題があった。
However, when voltage is applied to the electrodes to make one light-emitting layer emit light, dielectric breakdown occurs locally around pinholes, dust, defects, etc. in the film, and the breakdown spreads to the entire EL pixel (propagating breakdown). There was a problem in that the display quality of the panel was significantly deteriorated due to pixel loss (also called pixel loss).

本発明は上記従来の問題点に鑑みて成されたもので、絶
縁破壊のメカニズムを検討し、適当な電極材質を選択す
ることにより、絶縁耐圧の高い信頼性のある透明型EL
パネルや多色ELパネルを実現することを目的とする。
The present invention has been made in view of the above-mentioned conventional problems, and by studying the mechanism of dielectric breakdown and selecting appropriate electrode materials, it is possible to create a highly reliable transparent EL device with high dielectric strength.
The purpose is to realize panels and multicolor EL panels.

く課題を解決するための手段〉 上記従来技術の課題を解決する為の本発明の構成は、請
求項1においては絶縁性基板上に少なくとも一層のEL
発光層および絶縁層を挟んで積層された電極からなり、
前記電極に交流電圧を印加することにより前記発光層を
発光させる様にした薄膜EL素子において、前記電極の
内の少なくとも一層は透明で、かつ、前記発光層および
絶縁層からなる部分の融点より低融点の部材を用いたこ
とを特徴とするものであり。
Means for Solving the Problems> In claim 1, the structure of the present invention for solving the problems of the prior art is as follows:
Consists of laminated electrodes with a light-emitting layer and an insulating layer in between,
In a thin film EL device in which the light emitting layer is made to emit light by applying an alternating current voltage to the electrode, at least one layer of the electrode is transparent and has a melting point lower than that of the portion consisting of the light emitting layer and the insulating layer. It is characterized by using a member with a melting point.

請求項2においては請求項1記載の薄膜EL素子におい
て、低融点の部材はCTOとされ、そのCTOは5n0
2または5n02に添加物を加えた薄膜で挟まれている
ことを特徴とするものであり。
In claim 2, in the thin film EL element according to claim 1, the low melting point member is CTO, and the CTO is 5n0.
It is characterized by being sandwiched between thin films containing 2 or 5n02 and an additive.

請求項3においては請求項1記載の薄膜EL素子におい
て9発光層を2Nとし基板側からの電極を第1.第2.
第3電極とした場合、少なくとも前記第1.第2電極を
C’l’ Oとしたことを特徴とするものであり 請求項4においては請求項1記載の薄膜EL素子におい
て1発光層を2層とし基板側からの電極を第1.第2.
第3電極とした場合、少なくとも前記第2電極をCTO
とし、前記EL素子完成後前記第2電極に負の電位、他
の電極に正の直流電圧を印加した後、交流電圧を印加す
る様にしたことを特徴とするものであり。
In a third aspect of the present invention, in the thin film EL device according to the first aspect, the nine light emitting layers are 2N, and the electrodes from the substrate side are the first and second electrodes. Second.
When the third electrode is used, at least the first electrode. According to a fourth aspect of the present invention, in the thin film EL device according to claim 1, one light-emitting layer is made of two layers, and the electrode from the substrate side is made of C'l'O. Second.
When the third electrode is used, at least the second electrode is CTO.
After the EL element is completed, a negative potential is applied to the second electrode, a positive DC voltage is applied to the other electrodes, and then an AC voltage is applied.

請求項5においては請求項1記載の薄膜El素子におい
て1発光層を上部発光層と下部発光層の2層とし基板側
からの電極を第1.第2.第3電極とした場合、少なく
とも前記第1電極をCTO。
In a fifth aspect of the present invention, in the thin film El element according to the first aspect, one light emitting layer is made of two layers, an upper light emitting layer and a lower light emitting layer, and the electrodes from the substrate side are arranged as the first and second light emitting layers. Second. When the third electrode is used, at least the first electrode is CTO.

第2電極をI’f”Oとし、前記EL素子完成後前記第
2電極に正の電位、他の電極に負の直流電圧を印加した
後、交流電圧を印加する様にしたことを特徴とするもの
であり。
The second electrode is I'f"O, and after the EL element is completed, a positive potential is applied to the second electrode, a negative DC voltage is applied to the other electrodes, and then an AC voltage is applied. It is something to do.

請求項6においては請求項1記載の薄膜EL素子におい
て、少なくとも2層の発光層を形成する場合は、第1層
の発光が可能な状態まで製作した時点で一旦発光試験を
行った後、以降の製造工程を実行することを特徴とする
ものである。
In claim 6, in the thin film EL device according to claim 1, when at least two light emitting layers are formed, a light emitting test is performed once the first layer is manufactured to a state where it can emit light, and then thereafter. It is characterized by carrying out the manufacturing process of.

く作用〉 請求項1.3項において、電極の一方に発光層および絶
縁層からなる部分の融点より低融点の部材を用いれば1
発光層や絶縁層に欠陥があり、電圧印加によりその部分
が溶融しても一方の電極が溶融し、そこで発光層の溶融
はストップする(もし9両方の電極とも発光層および絶
縁層の融点より高融点の部材を用いた場合は溶融が全体
に拡がり発光か不可能になる)。
Effect> In claim 1.3, if a member having a melting point lower than the melting point of the portion consisting of the light-emitting layer and the insulating layer is used for one of the electrodes, 1.
Even if there is a defect in the emissive layer or insulating layer and that part melts when a voltage is applied, one electrode will melt and the emissive layer will stop melting (9) If both electrodes are below the melting point of the emissive layer and insulating layer, If a material with a high melting point is used, the melting will spread throughout, making it impossible to emit light.)

請求項2において、CTOは絶縁層からの酸素の影響で
抵抗が増大する。SnO2やこれに添加物を加えたもの
は低抵抗のものを形成するのは雑しいが酸素や水への耐
性が強いのでこれでCTOを挾む事により抵抗の増大を
阻止することが出来る。
In claim 2, the resistance of the CTO increases due to the influence of oxygen from the insulating layer. Although it is difficult to form a low-resistance product with SnO2 or additives added thereto, it has strong resistance to oxygen and water, so by sandwiching CTO with this, it is possible to prevent an increase in resistance.

請求項4において、第2の電極であるCTOに負の電圧
を他の電極に正の電圧を印加することにより予め局部的
な破壊を起こしておけば、破壊が全体に広がる事がない
。
In claim 4, if local destruction is caused in advance by applying a negative voltage to the second electrode, CTO, and a positive voltage to the other electrodes, the destruction will not spread to the entire area.

請求項5において第2電極であるITOに正の電位、他
の電極に負の直流電圧を印加することにより予め局部的
な破壊を起こしておけば、破壊が全体に広がる事がない
。
In claim 5, if local destruction is caused in advance by applying a positive potential to the ITO, which is the second electrode, and a negative DC voltage to the other electrodes, the destruction will not spread to the whole.

請求項6において、下部発光層を製作した時点で破壊検
査をすれば、下部発光層の破壊の影響が上部発光層まで
及ぶことかない。
In claim 6, if a destructive inspection is performed at the time when the lower light emitting layer is manufactured, the influence of destruction of the lower light emitting layer does not extend to the upper light emitting layer.

〈実施例〉 以下1図面に従い本発明の一実施例を説明する。<Example> An embodiment of the present invention will be described below with reference to one drawing.

はじめに第1電極をITOとし、第2電極としてAIを
用いた場合とITOを用いた場合における絶縁破壊の原
因について説明する。薄膜EL素子はガラス基板上にT
TO電極、絶縁層9発光層。
First, the causes of dielectric breakdown in the cases where ITO is used as the first electrode and AI is used as the second electrode, and when ITO is used as the second electrode will be explained. The thin film EL element is mounted on a glass substrate.
TO electrode, insulating layer 9 light emitting layer.

絶縁層およびAj7電極をスパッタ法や蒸着等の薄膜形
成手段により形成するか1発光層を発光させようとして
これを挾む電極に電圧を印加した場合。
When the insulating layer and the Aj7 electrode are formed by a thin film forming method such as sputtering or vapor deposition, or when a voltage is applied to the electrodes sandwiching the light-emitting layer in order to cause it to emit light.

各層のいずれかにゴミや欠陥等があると局所的に絶縁破
壊が発生し、第1電極、絶縁層1発光層および第2電極
が溶融する(この溶融状態においては絶縁層および発光
層の絶縁性が低下し導通状態となる)。
If there is dust or defects in any of the layers, dielectric breakdown occurs locally, and the first electrode, the insulating layer 1, the light-emitting layer, and the second electrode melt (in this melted state, the insulation of the insulating layer and the light-emitting layer conductivity decreases and becomes conductive).

第9図は第1電極をITO,第2電極をAIとして電圧
を印加した場合の破壊の状態を示す拡大断面図である。
FIG. 9 is an enlarged sectional view showing the state of destruction when a voltage is applied using ITO as the first electrode and AI as the second electrode.

電圧を次第に上昇させていくと膜に欠陥等があった場合
、絶縁材料の本来有する絶縁耐圧値より低い電圧でAI
電極、絶縁層および発光層が破壊されて導通した状態と
なり1局部的に溶融するが、絶縁層やI’f’Oより融
点の低いAIがはじめに溶解、蒸発する(即ち、絶縁層
を残したままその上のAI(Aで示す部分))が溶融す
る。従ってその部分の絶縁状態はすぐ回復し。
When the voltage is gradually increased, if there is a defect in the film, AI will be removed at a voltage lower than the dielectric strength value originally possessed by the insulating material.
The electrode, insulating layer, and light-emitting layer are destroyed and become conductive, melting locally, but AI, which has a lower melting point than the insulating layer and I'f'O, melts and evaporates first (that is, the insulating layer is left behind). The AI above it (the part indicated by A) will melt. Therefore, the insulation state of that part will recover quickly.

絶縁層の溶融は持続せず局所的に止まって画素全体に波
及しない。そのため、ELデイスプレィとしての機能は
持続される。
The melting of the insulating layer does not last, stops locally, and does not spread to the entire pixel. Therefore, the function as an EL display is maintained.

第10図は第1.第2電極をITOとした場合の破壊の
状態を示す拡大断面図である。この場合も、絶縁層中に
存在するゴミや欠陥によりITOおよび発光層を含む絶
縁層が溶融するが、I’l’0の溶融温度が絶縁層と等
しいかそれよりも高いので、その溶解、蒸発の速度は絶
縁層よりも遅くなる。そのため、絶縁層は高温による導
通状態を維持したまま矢印方向に溶解による破壊が次々
と連続して発生し、ついにはその画素が破壊してしよつ 第11図はガラス基板の上に第1.電極としてIToを
使用し、絶縁層としてS i 02 、 Ta205、
Al2ozの各絶縁層を0.3〜0.5μm程度に形成
し、第2電極としてAIまたはITOを使用して伝搬型
破壊に至る電界強度を試験した結果を示すものである。
Figure 10 shows 1. FIG. 7 is an enlarged cross-sectional view showing a state of destruction when the second electrode is made of ITO. In this case as well, the insulating layer including ITO and the light-emitting layer melts due to dust and defects existing in the insulating layer, but since the melting temperature of I'l'0 is equal to or higher than that of the insulating layer, its melting and The rate of evaporation will be slower than that of the insulating layer. As a result, the insulating layer continues to melt and break down in the direction of the arrow while maintaining its conductive state due to the high temperature, and finally the pixel is destroyed. .. ITo is used as the electrode, and Si02, Ta205, and insulating layer are used.
The results show the results of testing the electric field strength leading to propagation type breakdown by forming each insulating layer of Al2oz to a thickness of about 0.3 to 0.5 μm and using AI or ITO as the second electrode.

図によれば、絶縁層としてSiO2を使用し第2電極と
してAIを使用した場合は7.6X10’V/cm程度
の耐圧があり、ITOを使用した場合は2.lX10’
V/cm程度の耐圧しかない。また、絶縁層としてTa
205を使用した場合はAIの場合はIXl 06V/
cm、IToの場合は0 、5 X 10 ’ V /
 c m程度、また、絶縁層としてA11203を使用
した場合はAIの場合は4.8X10’ V/cm、I
TOの場合は08X10’V/cm程度の耐圧しかない
。先に述べた様に発光層を発光させるためには1〜2×
IQ’V/cm程度の電界が必要なので、絶縁層の絶縁
耐圧としては充分な余裕が必要である。従って第2電極
をITOとした場合はいずれの絶縁層を使用しても伝搬
型破壊が生ずることになる。
According to the figure, when SiO2 is used as the insulating layer and AI is used as the second electrode, the withstand voltage is about 7.6 x 10'V/cm, and when ITO is used, the breakdown voltage is about 2. lX10'
The withstand voltage is only about V/cm. In addition, as an insulating layer, Ta
If you use 205, if you use AI, IXl 06V/
cm, 0 for ITo, 5 x 10' V/
cm, and when A11203 is used as the insulating layer, 4.8X10' V/cm for AI, I
In the case of TO, the withstand voltage is only about 08×10'V/cm. As mentioned earlier, in order to make the light emitting layer emit light, the
Since an electric field of approximately IQ'V/cm is required, a sufficient margin is required for the dielectric strength voltage of the insulating layer. Therefore, if the second electrode is made of ITO, propagation type breakdown will occur no matter which insulating layer is used.

ここで A1.ITO,発光層および絶縁層の融点につ
いてみるとAIの融点は660℃、ITOの融点は16
00〜2000℃であり、ZnSを主成分とする発光層
の昇華点(ZnSは昇華性物質なので)は1180℃程
度、また。絶縁層の5i02の融点は1610〜171
0℃、Ta205は1470℃、Al2O3は2050
℃である。
Here A1. Looking at the melting points of ITO, the light emitting layer, and the insulating layer, the melting point of AI is 660°C, and the melting point of ITO is 16
00 to 2000°C, and the sublimation point of the light-emitting layer mainly composed of ZnS (since ZnS is a sublimable substance) is about 1180°C. The melting point of 5i02 in the insulating layer is 1610-171
0℃, Ta205 is 1470℃, Al2O3 is 2050℃
It is ℃.

以上のことから第1.第2電極を共にITOとした場合
は9発光層および絶縁層からなる部分より電極の方が融
点が高いので伝搬型破壊が進行することが分る。
From the above, the first point. It can be seen that when both the second electrodes are made of ITO, the melting point of the electrodes is higher than that of the part consisting of the light emitting layer and the insulating layer, so propagation-type breakdown progresses.

本出願人は以上の事実を実験により確認し9発光層およ
び絶縁層からなる部分より融点が低く。
The present applicant confirmed the above fact through experiments, and found that the melting point is lower than that of the part consisting of the light-emitting layer and the insulating layer.

かつ、透明性があり、比抵抗か小さく、スペクトルの吸
収が少なく、パターン形成か容易な物質について種々検
討した。その結果Cd Oおよび5n02を主成分とす
る混合物(Cd2Sn04やCd5n03・・・以下、
共にCTOという)か透明型EL電極としてずぐれてい
ることを発見した。
In addition, various studies were conducted on materials that are transparent, have low resistivity, have low spectral absorption, and are easy to pattern. As a result, a mixture containing CdO and 5n02 as main components (Cd2Sn04, Cd5n03...hereinafter,
We discovered that it is superior as a transparent EL electrode (both referred to as CTO).

第1図は本発明の請求項1における一実施例を示すEL
発光素子の要部断面図であり、第2電極としてCTOを
用いている他は第8図の従来例と同様である。
FIG. 1 shows an EL device according to an embodiment of claim 1 of the present invention.
8 is a sectional view of a main part of a light emitting element, which is the same as the conventional example shown in FIG. 8, except that CTO is used as the second electrode.

CTOの融点は1130℃程度であり、これを第2電極
として前記第11図に示す3種の絶縁層を用いて実験し
た所いずれもI T Oの場合に比較して2〜3倍の伝
搬型破壊の電界強度を得ることが出来、透明型フラット
パネルを実現することが出来た。
The melting point of CTO is about 1130°C, and when we conducted experiments using CTO as the second electrode and the three types of insulating layers shown in Figure 11 above, the propagation was 2 to 3 times that of ITO. We were able to obtain the electric field strength that would break the mold, and we were able to realize a transparent flat panel.

なお、第2電極としては上記c ’r oに限ることな
く例えば酸化膜としての100%CdO(700℃で昇
華)、SnO2(1127℃で溶融)も可能であり、ま
た、5n02に添加物を加えたものも可能である。例え
ば、Sbを加えたもの(ATo)やFを加えたもの(F
TO)や、同じく5n02に添加物としてPまなはTe
またはC1を加えたもの等である。その他CuI、Cu
2 Sχ等も用いることが可能であり、要は透明性があ
り。
Note that the second electrode is not limited to the above-mentioned c'ro, and for example, 100% CdO (sublimated at 700°C) or SnO2 (melted at 1127°C) as an oxide film is also possible, and additives may be added to 5n02. Additions are also possible. For example, those with Sb added (ATo) and those with F added (FTo).
TO) and also Pmanah Te as an additive to 5n02.
Or, it is the one in which C1 is added. Other CuI, Cu
2 Sχ etc. can also be used, and the key is transparency.

比抵抗が小さく発光層および絶縁層からなる部分の融点
より低融点の部材であればよい。
Any member may be used as long as it has a low specific resistance and a melting point lower than that of the portion consisting of the light emitting layer and the insulating layer.

第2図は請求項1における他の実施例を示すもので1本
発明を2層の発光層を有するEL素子に適用した断面図
である。図において1はガラス基板、2は第1電極(C
TO)、3,5,7.9は絶縁層、4は下部発光層、6
は第2電極(ITO)、8は上部発光層、10は第3電
極(CTO)である。ここで上部発光層8は例えばZn
S :TbF3などの緑色のEL素子が用いられ、下部
発光層4はZnS : SmF3等の赤色EL素子が用
いられる。
FIG. 2 shows another embodiment of claim 1, and is a sectional view in which the present invention is applied to an EL element having two light emitting layers. In the figure, 1 is a glass substrate, 2 is a first electrode (C
TO), 3, 5, 7.9 are insulating layers, 4 is a lower light emitting layer, 6
is a second electrode (ITO), 8 is an upper light emitting layer, and 10 is a third electrode (CTO). Here, the upper light emitting layer 8 is made of, for example, Zn.
A green EL element such as S:TbF3 is used, and the lower light emitting layer 4 is a red EL element such as ZnS:SmF3.

上記構成によればITOからなる第2電極を挟んでCT
Oからなる第1.第3電極か形成されているので、絶縁
破壊があってもその破壊は局部的に押えることが出来る
ので、透明なパネルに多色の発光素子を発光させること
が可能となる。
According to the above configuration, CT is performed across the second electrode made of ITO.
1st consisting of O. Since the third electrode is formed, even if dielectric breakdown occurs, the breakdown can be suppressed locally, making it possible to emit light from multicolored light emitting elements on a transparent panel.

第3図は請求項2における実施例を示すものである。本
出願人の実験によればCTOは融点の低い電極としては
優れているか、絶縁層等からの酸素の影響を受けやすく
(酸素を吸収したり放出する)抵抗値の上昇や透明度が
低下するという問題がある。一方5n02またはSnO
2に添加物を加えた(以下、ATOという)部材は融点
はCTO並で、酸素や水への耐性が強いという利点があ
るが低抵抗のものを形成しにくいという問題かある。そ
こで1本発明ではCTOを〜2000A程度とし、これ
を〜500A程度のATOで挟んだものである。
FIG. 3 shows an embodiment according to claim 2. According to the applicant's experiments, CTO is either superior as an electrode with a low melting point, or is susceptible to the influence of oxygen from insulating layers (absorbing and releasing oxygen), resulting in an increase in resistance and a decrease in transparency. There's a problem. while 5n02 or SnO
A material made by adding additives to No. 2 (hereinafter referred to as ATO) has a melting point similar to that of CTO, and has the advantage of being highly resistant to oxygen and water, but has the problem of being difficult to form into a material with low resistance. Therefore, in one aspect of the present invention, the CTO is set to about 2000A, which is sandwiched between ATOs of about 500A.

上記構成によれば低抵抗が得やすいCTOを低抵抗は得
にくいが酸素や水への耐性の強いA ’I” 0で保護
するので抵抗値の上昇や透明度の低下のない電極を得る
ことが出来る。
According to the above configuration, since the CTO, which is easy to obtain low resistance, is protected by A'I"0, which is difficult to obtain low resistance but has strong resistance to oxygen and water, it is possible to obtain an electrode without an increase in resistance value or a decrease in transparency. I can do it.

第4図は請求項3における一実施例を示すもので、第2
図に示す2層のEL素子において第1電極、第2電極を
CTOとしたものである。
FIG. 4 shows an embodiment according to claim 3, and shows the second embodiment.
In the two-layer EL element shown in the figure, the first electrode and the second electrode are CTO.

−1−記梢成によれば第2図の例に比較して絶縁破壊は
さらに局部的となる。
-1- According to the configuration described above, dielectric breakdown becomes more localized than in the example shown in FIG.

第5図は請求項4における一実施例を示すもので、第2
図に示す2層のE L素子において第2電極をCTOと
し、第1.第3電極をITO電極としたものであり1本
発明ではEL素子完成後第2電極に負の電圧を他の電極
に正の電圧を印加することにより絶縁破壊があってもそ
の破壊を局部的にとどめる様にしたものである。
FIG. 5 shows an embodiment according to claim 4, and shows the second embodiment.
In the two-layer EL element shown in the figure, the second electrode is CTO, and the first electrode is CTO. The third electrode is an ITO electrode. 1. In the present invention, after the EL element is completed, by applying a negative voltage to the second electrode and a positive voltage to the other electrodes, even if dielectric breakdown occurs, the breakdown can be localized. It was designed to remain at .

第6図は請求項5における一実施例を示すもので、第2
図に示す2層のEL素子において第2電極を工TOとし
、第1.第3電極をCTO電極としたものであり1本発
明ではEL素子完成後第2電極に正の電圧を他の電極に
負の電圧を印加することにより絶縁破壊があってもその
破壊を局部的にとどめる様にしたものである。
FIG. 6 shows an embodiment according to claim 5, and shows the second embodiment.
In the two-layer EL element shown in the figure, the second electrode is TO and the first electrode is TO. The third electrode is a CTO electrode, and in the present invention, after the EL element is completed, by applying a positive voltage to the second electrode and a negative voltage to the other electrodes, even if dielectric breakdown occurs, the breakdown can be localized. It was designed to remain at .

なお、請求項4.5における電極の組み合わせと印加電
圧の関係については本出願人が実験により確認したこと
であるが、理論的な解明までにはいたっていない。
The relationship between the electrode combination and the applied voltage in claim 4.5 has been confirmed by the applicant through experiments, but has not yet been theoretically elucidated.

第7図は請求項6の説明に用いる図であり、ここでは第
1電極をTTO,第2電極をCT Oとしここまで製作
した時点で第1電極に距、第2電極に負の電圧を印加し
て破壊試験を行う。その破壊試験によりゴミや欠陥があ
る部分は局部的に破壊する(12は下部発光層の破壊に
より生じた穴を示している)。その後第2電極(CTO
)の全体に絶縁層を施して破壊した部分を埋めるととも
に分離平坦化層13を形成する。その後は従来と同様節
2の発光層8を挟んで絶縁層7.9および第2電極6a
、第3t′Fi110を形成する。その場合第2電極2
aと第3電極10のいずれかはCT Oを用いたほうか
望ましい。」−記製造方法によれは第1発光層の破壊の
影響か第2発光層まで及んで破壊されることかなくなる
ので表示品質の向」二をはかることか出来る。
FIG. 7 is a diagram used to explain claim 6, and here, the first electrode is TTO, the second electrode is CTO, and at the time of manufacturing up to this point, a distance is applied to the first electrode, and a negative voltage is applied to the second electrode. Apply the voltage and perform a destructive test. Through the destructive test, parts with dust or defects are locally destroyed (numeral 12 indicates a hole caused by destruction of the lower light emitting layer). Then the second electrode (CTO
), an insulating layer is applied to the entire area to fill in the broken portion and to form an isolation planarization layer 13. After that, the insulating layer 7.9 and the second electrode 6a are sandwiched between the light emitting layer 8 of node 2 and the second electrode 6a as in the conventional case.
, a third t'Fi 110 is formed. In that case, the second electrode 2
It is preferable to use CTO for either a or the third electrode 10. According to the manufacturing method described above, since the influence of destruction of the first light emitting layer does not extend to the second light emitting layer and destroying it, it is possible to improve the display quality.

なお9発光層を3層とする場合も電極をすべてCTOと
することにより絶縁破壊を局部的に押えることか出来る
。更に2発光層は2層または3層であるか透明性を必要
としない場合は最端の電極(背面型@l)はAI電極を
用いることか出来る。
Note that even when the nine light-emitting layers are made up of three layers, dielectric breakdown can be locally suppressed by making all the electrodes CTO. Furthermore, if the two light-emitting layers are two or three layers, or transparency is not required, an AI electrode may be used as the outermost electrode (back type @l).

〈発明の効果〉 以上実施例とともに具体的に説明した様に本発明によれ
ば1発光層を挾む電極の内の少なくとも一層は透明で、
かつ1発光層および絶縁層からなる融点より低融点の部
材を用いたので、フラットパネル全体に絶縁破壊が広が
らない透明パネルを実現することか出来る。また、CT
Oの配置や予め直流電圧を印加したり、工程の途中に試
験工程を設けることにより信頼性の高いEL発光素子を
実現する事が出来る。
<Effects of the Invention> As specifically explained above in conjunction with the embodiments, according to the present invention, at least one layer of the electrodes sandwiching one light-emitting layer is transparent,
In addition, since a member having a melting point lower than that of one light-emitting layer and an insulating layer is used, it is possible to realize a transparent panel in which dielectric breakdown does not spread over the entire flat panel. Also, CT
A highly reliable EL light emitting device can be realized by arranging O, applying a DC voltage in advance, and providing a test step in the middle of the process.

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

第1図は本発明の請求項1に関する薄膜EL素子の一実
施例を示す断面図、第2図は請求項1に関する他の実施
例を示す断面図、第3図は本発明の請求項2に関する薄
膜EL素子の一実施例を示す断面図、第4図は本発明の
請求項3に関する薄膜E L、素子の一実施例を示す断
面図、第5図は本発明の請求項4に関する薄膜EI−素
子の一実施例を示す断面図、第6図は本発明の請求項5
に関する薄膜EL素子の一実施例を示す断面図、第7図
は本発明の請求項6に関する薄膜E L素子の一実施例
を示す断面図、第8図は従来のEI−薄膜素子を示す断
面図、第9図、第10図は電圧印加により局部的に溶融
か発生した状態を示す断面図、第11図は絶縁層の材質
と伝搬型破壊の電界強度の関係を示す図である。
FIG. 1 is a sectional view showing one embodiment of a thin film EL element related to claim 1 of the present invention, FIG. 2 is a sectional view showing another embodiment related to claim 1, and FIG. 3 is a sectional view showing another embodiment of the thin film EL element related to claim 1 of the present invention. FIG. 4 is a sectional view showing an embodiment of a thin film EL element according to claim 3 of the present invention, and FIG. A cross-sectional view showing one embodiment of the EI-element, FIG. 6 is a fifth aspect of the present invention.
7 is a sectional view showing an embodiment of a thin film EL element according to claim 6 of the present invention, and FIG. 8 is a sectional view showing a conventional EI thin film element. 9 and 10 are cross-sectional views showing a state in which local melting occurs due to voltage application, and FIG. 11 is a diagram showing the relationship between the material of the insulating layer and the electric field strength of propagation type breakdown.

Claims (1)

【特許請求の範囲】 1)絶縁性基板上に少なくとも一層のEL発光層および
絶縁層を挟んで積層された電極からなり,前記電極に交
流電圧を印加することにより前記発光層を発光させる様
にした薄膜EL素子において前記電極の内の少なくとも
一層は透明で,かつ,前記発光層および絶縁層からなる
部分の融点より低融点の部材を用いたことを特徴とする
薄膜EL素子。 2)請求項1記載の薄膜EL素子において,低融点の部
材はCTOとされ,そのCTOはSnO_2またはSn
O_2に添加物を加えた薄膜で挟まれていることを特徴
とする薄膜EL素子。 3)請求項1記載の薄膜EL素子において,発光層を上
部発光層と下部発光層の2層とし基板側からの電極を第
1,第2,第3電極とした場合,少なくとも前記第1,
第2電極をCTOとしたことを特徴とする薄膜EL素子
。 4)請求項1記載の薄膜EL素子において,発光層を上
部発光層と下部発光層の2層とし基板側からの電極を第
1,第2,第3電極とした場合,少なくとも前記第2電
極をCTOとし,前記EL素子完成後前記第2電極に負
の電位,他の電極に正の直流電圧を印加した後,交流電
圧を印加する様にしたことを特徴とする薄膜EL素子の
製造方法。 5)請求項1記載の薄膜EL素子において,発光層を上
部発光層と下部発光層の2層とし基板側からの電極を第
1,第2,第3電極とした場合,少なくとも前記第1電
極をCTO,第2電極をITOとし,前記EL素子完成
後前記第2電極に正の電位,他の電極に負の直流電圧を
印加した後,交流電圧を印加する様にしたことを特徴と
する薄膜EL素子の製造方法。 6)請求項1記載の薄膜EL素子において,少なくとも
2層の発光層を形成する場合は,第1層の発光が可能な
状態まで製作した時点で一旦発光試験を行った後,以降
の製造工程を実行することを特徴とする薄膜EL素子の
製造方法。
[Scope of Claims] 1) Consisting of an electrode laminated on an insulating substrate with at least one EL light emitting layer and an insulating layer sandwiched therebetween, the light emitting layer is made to emit light by applying an alternating current voltage to the electrode. 1. A thin film EL device characterized in that at least one of the electrodes is transparent and has a melting point lower than that of the light emitting layer and the insulating layer. 2) In the thin film EL device according to claim 1, the low melting point member is CTO, and the CTO is SnO_2 or Sn
A thin film EL device characterized by being sandwiched between thin films containing O_2 and additives. 3) In the thin film EL device according to claim 1, when the light emitting layer has two layers, an upper light emitting layer and a lower light emitting layer, and the electrodes from the substrate side are first, second, and third electrodes, at least the first, second, and third light emitting layers are provided.
A thin film EL device characterized in that the second electrode is CTO. 4) In the thin film EL device according to claim 1, when the light-emitting layer has two layers, an upper light-emitting layer and a lower light-emitting layer, and the electrodes from the substrate side are the first, second, and third electrodes, at least the second electrode A method for manufacturing a thin film EL device, characterized in that after completion of the EL device, a negative potential is applied to the second electrode, a positive DC voltage is applied to the other electrodes, and then an AC voltage is applied. . 5) In the thin film EL device according to claim 1, when the light-emitting layer has two layers, an upper light-emitting layer and a lower light-emitting layer, and the electrodes from the substrate side are first, second, and third electrodes, at least the first electrode is CTO, the second electrode is ITO, and after the EL element is completed, a positive potential is applied to the second electrode, a negative DC voltage is applied to the other electrodes, and then an AC voltage is applied. A method for manufacturing a thin film EL element. 6) In the thin film EL device according to claim 1, when at least two light emitting layers are formed, a light emitting test is performed once the first layer is manufactured to a state where it can emit light, and then the subsequent manufacturing steps are performed. A method for manufacturing a thin film EL device, characterized by carrying out the following steps.
JP1276718A 1988-12-02 1989-10-24 Thin film EL device and method of manufacturing the same Expired - Fee Related JP2838111B2 (en)

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JP30580788 1988-12-02
JP63-305807 1988-12-02
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WO2006077767A1 (en) * 2005-01-21 2006-07-27 Pioneer Corporation Organic el element manufacturing method and organic el element obtained by the same

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