JPH0524155Y2 - - Google Patents
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- Publication number
- JPH0524155Y2 JPH0524155Y2 JP1986095583U JP9558386U JPH0524155Y2 JP H0524155 Y2 JPH0524155 Y2 JP H0524155Y2 JP 1986095583 U JP1986095583 U JP 1986095583U JP 9558386 U JP9558386 U JP 9558386U JP H0524155 Y2 JPH0524155 Y2 JP H0524155Y2
- Authority
- JP
- Japan
- Prior art keywords
- panel
- back electrode
- insulating film
- film
- hole
- Prior art date
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Description
【考案の詳細な説明】
(産業上の利用分野)
この考案はエレクトロルミネツセンスパネル、
特に交流形薄膜2重絶縁構造のエレクトロルミネ
ツセンスパネルの背面電極の厚みに関する。[Detailed explanation of the invention] (Industrial application field) This invention is an electroluminescent panel,
In particular, it relates to the thickness of the back electrode of an electroluminescent panel having an AC type thin film double insulation structure.
(従来の技術)
従来より、大型表示装置に適用して好適な交流
形薄膜2重絶縁構造のエレクトロルミネツセンス
パネル(以下、単にELパネルと称する)につい
ての研究及び開発が行われており、例えば、以下
の文献に開示されている。(Prior Art) Research and development have been conducted on electroluminescent panels (hereinafter simply referred to as EL panels) having an AC type thin film double insulation structure suitable for application to large display devices. For example, it is disclosed in the following documents.
文献:信学技報、82(68)CPM82−10、P15〜
17(1982年6月25日)電子通信学会
文献:日本学術振興会、光電相互変換第125委
員会、第109回資料第416号、P7(昭59年2月24
日)
文献:日本学術振興会、光電相互変換第125委
員会、第109回資料第418号、P18(昭59年2月
24日)
文献:エスアイデイ81ダイジエスト(SID 81
DIGEST)、P22〜23
文献:エスアイデイ83ダイジエスト(SID 83
DIGEST)、P141〜142
文献:プロシーデイング オブ ザ エスアイ
デイ(Proceeding of the SID)、24/2、
P120〜121。Literature: IEICE Technical Report, 82 (68) CPM82-10, P15~
17 (June 25, 1982) IEICE Literature: Japan Society for the Promotion of Science, 125th Committee on Photoelectric Interconversion, 109th Material No. 416, P7 (February 24, 1982)
(Japanese) Literature: Japan Society for the Promotion of Science, 125th Committee on Photoelectric Interconversion, 109th Meeting Material No. 418, P18 (February 1982)
24th) Literature: SID 81 Digest (SID 81
DIGEST), P22-23 Literature: SID 83 Digest (SID 83
DIGEST), P141-142 Literature: Proceedings of the SID, 24/2,
P120-121.
この考案のELパネルの説明に先立ち、従来の
ELパネルにつき説明する。 Before explaining the EL panel of this invention, we will explain the conventional EL panel.
I will explain about the EL panel.
第4図はこのような従来のELパネルの代表的
な発光素子の部分の構造を概略的に示す要部断面
図(断面を示すハツチング等は省略してある。)
である。第4図において、10はガラス基板、1
2はこのガラス基板10上に設けられた例えば
ITOからなる透明電極である。14はこの透明電
極12上に設けられた第一絶縁膜で、例えば、透
明電極12側から厚み1000ÅのSiO2(二酸化珪
素)膜と、その上側の厚み3000ÅのTa2O5(五酸
化タンタル)膜との二重膜構造となつている。こ
の第一絶縁膜14上に発光膜16を具え、例え
ば、この発光膜16をZnS:Mn(硫化亜鉛マンガ
ン)を以つて膜厚6000Åに構成し、この発光膜1
6上に第一絶縁膜14と同じ材料から成り同様に
構成された第二絶縁膜18を設け、この絶縁膜1
8の上側にA(アルミニウム)で形成した背面
電極20を設けた構造となつている。 FIG. 4 is a cross-sectional view of the main part schematically showing the structure of a typical light emitting element of such a conventional EL panel (hatching etc. indicating the cross section are omitted).
It is. In FIG. 4, 10 is a glass substrate, 1
2 is provided on this glass substrate 10, for example.
A transparent electrode made of ITO. Reference numeral 14 denotes a first insulating film provided on the transparent electrode 12, for example, a SiO 2 (silicon dioxide) film with a thickness of 1000 Å from the transparent electrode 12 side and a Ta 2 O 5 (tantalum pentoxide) film with a thickness of 3000 Å on the upper side. ) has a double membrane structure with a membrane. A light-emitting film 16 is provided on the first insulating film 14, and for example, the light-emitting film 16 is made of ZnS:Mn (zinc manganese sulfide) with a thickness of 6000 Å.
A second insulating film 18 made of the same material and having the same structure as the first insulating film 14 is provided on the first insulating film 14.
It has a structure in which a back electrode 20 made of A (aluminum) is provided on the upper side of the electrode 8 .
このような構造のELパネルの透明電極12と、
背面電極20との間に交流電圧を継続的に印加さ
せると、発光膜16が発光を開始する。ELパネ
ルのこの発光を図中矢印22で示した方向から目
視することが出来る。 The transparent electrode 12 of the EL panel having such a structure,
When an AC voltage is continuously applied between the back electrode 20 and the back electrode 20, the light emitting film 16 starts emitting light. This light emission from the EL panel can be visually observed from the direction indicated by arrow 22 in the figure.
この構造のELパネルにおいては、第一絶縁膜
14、発光膜16及び第二絶縁膜18の少なくと
もいずれかの膜が何等かの原因により部分的に剥
離していたり或は塵埃が付着していたりするよう
な欠陥があると、交流電圧の印加時に第一絶縁膜
14、発光膜16及び第二絶縁膜18を通して破
壊して直径d1が約30〜60μmの穴24が開き、ま
た、ITO透明電極12よりも融点の低いアルミニ
ウム背面電極20にも直径d2の穴26が開いてし
まう。このような破壊穴24及び26の様子を概
略的に第5図に要部断面図(断面を示すハツチン
グ等は省略してある。)として示した。 In the EL panel having this structure, at least one of the first insulating film 14, the light-emitting film 16, and the second insulating film 18 may be partially peeled off for some reason, or dust may be attached to it. If such a defect exists, it will break through the first insulating film 14, the light-emitting film 16, and the second insulating film 18 when an AC voltage is applied, and a hole 24 with a diameter d1 of about 30 to 60 μm will open, and the ITO transparent The aluminum back electrode 20, which has a lower melting point than the electrode 12, also has a hole 26 with a diameter d2 . The appearance of such fractured holes 24 and 26 is schematically shown in FIG. 5 as a cross-sectional view of the main part (hatching etc. indicating the cross section are omitted).
ところで、各文献に開示されている構造のEL
パネルついて、背面電極厚tと積層厚Tとの膜厚
比(t/T)を調べたところ、次の表に示す結
果が得られた。 By the way, the EL structure disclosed in each document
When the thickness ratio (t/T) between the back electrode thickness t and the lamination thickness T was investigated for the panel, the results shown in the following table were obtained.
表
文献名 t/T
文献 3000Å/14500Å=0.21
文献 500Å/15000Å=0.03
文献 200nm/1950nm=0.10
文献 1000Å/13000Å=0.08
文献 0.1μm/1.1μm =0.09
文献 1500Å/14000Å=0.11
この表からも理解出来るように、これら文献に
開示されたELパネルの背面電極20の厚みtと
積層厚Tと比t/Tはt/T=0.03〜0.21の範囲
にある。 Table Literature Name t/T Literature 3000Å/14500Å=0.21 Literature 500Å/15000Å=0.03 Literature 200nm/1950nm=0.10 Literature 1000Å/13000Å=0.08 Literature 0.1μm/1.1μm =0.09 Literature 1500Å/14000Å=0. 11 It can be understood from this table As such, the thickness t of the back electrode 20 of the EL panel disclosed in these documents, the lamination thickness T, and the ratio t/T are in the range of t/T=0.03 to 0.21.
この表に示された厚み関係にある各文献の
ELパネルにつき破壊穴24及び26の大きさを
調べたところ、全て穴径d1よりも大きな穴径d2の
破壊穴26が背面電極20に発生することが分か
つた。 For each document related to the thickness shown in this table,
When the sizes of the fracture holes 24 and 26 in the EL panel were investigated, it was found that the fracture holes 26, which had a hole diameter d2 larger than the hole diameter d1 , were all generated in the back electrode 20.
このような破壊膜24及び26の大きさ関係と
なる理由は、破壊時の瞬時の放電によつて第一絶
縁膜14、発光膜16及び第二絶縁膜18が発熱
気化すると同時に、背面電極20も発熱して中心
部が気化し、周囲の溶解部が表面張力によつて広
がることに起因して、穴直径d1よりも大きな穴直
径d2となるものと推測される。 The reason for the size relationship of the breakdown films 24 and 26 is that the first insulating film 14, the light-emitting film 16, and the second insulating film 18 are heated and vaporized by instantaneous discharge at the time of breakdown, and at the same time, the back electrode 20 It is presumed that the hole diameter d 2 is larger than the hole diameter d 1 due to heat generation and vaporization of the central portion, and the surrounding melted portion expanding due to surface tension.
第6図はこの破壊穴24及び26が生じたEL
パネルの動作を説明するための要部の概略的斜視
図である。この図からも理解出来るように、透明
電極12と、背面電極20との間に交流電圧を印
加すると、欠陥が生じていなければこれら電極の
交点が発光するが、前述したような破壊穴24よ
りも大きな破壊穴26が発生していると、通常は
直線状に形成されている背面電極20がその幅方
向に断線してしまい、その結果、ELパネルをマ
トリクス表示させることが出来ない。 Figure 6 shows the EL with these fracture holes 24 and 26.
FIG. 3 is a schematic perspective view of main parts for explaining the operation of the panel. As can be understood from this figure, when an AC voltage is applied between the transparent electrode 12 and the back electrode 20, the intersection of these electrodes will emit light if there is no defect, but the broken hole 24 as described above will emit light. If a large fracture hole 26 occurs, the back electrode 20, which is normally formed in a straight line, will be broken in the width direction, and as a result, the EL panel cannot display a matrix.
(考案が解決しようとする問題点)
このように、従来構造のELパネルでは、背面
電極の厚みtと第一絶縁膜、発光膜及び第二絶縁
膜の積層厚Tとの膜厚比t/Tがt/T=0.03〜
0.21の範囲内である場合には、積層に発生する穴
の直径d1よりも背面電極に発生する穴の直径d2の
方が大きくなるため、背面電極の断線を来し、こ
れがためELパネルの各画素を確実に発光させる
ことが出来ず、従つて高精細なマトリクス表示を
行うことが出来ないという問題点があつた。(Problem to be solved by the invention) As described above, in the EL panel of the conventional structure, the film thickness ratio t/ T is t/T=0.03~
If it is within the range of 0.21, the diameter d 2 of the hole created in the back electrode is larger than the diameter d 1 of the hole created in the lamination, resulting in disconnection of the back electrode, which causes the EL panel to fail. There was a problem in that each pixel in the display could not be made to emit light reliably, and therefore a high-definition matrix display could not be performed.
この考案は上述した従来の問題点に鑑み成され
たものであり、従つて、この考案の目的は穴直径
d1よりも穴直径d2が大きくなるという問題点を解
決して、背面電極に断線が生ぜず、しかも、表示
輝度ムラを生じないで高精細なマトリクス表示を
行うことが出来る構成にした交流形薄膜2重絶縁
構造のELパネルを提供することにある。 This invention was created in view of the problems of the conventional methods mentioned above, and therefore, the purpose of this invention is to improve the hole diameter.
This is an alternating current that solves the problem of the hole diameter d2 being larger than d1 , and has a structure that allows high-definition matrix display without causing disconnection in the back electrode and without causing display brightness unevenness. Our objective is to provide an EL panel with a thin film double insulation structure.
(問題点を解決するための手段)
この目的の達成を図るため、この考案による
ELパネルの構造によれば、背面電極がアルミニ
ウムよりなり、この背面電極の厚みをtとし及び
第一絶縁膜、発光膜及び第二絶縁膜の積層厚をT
としたとき、膜厚比t/Tをt/T≧0.5とする。(Means for solving the problem) In order to achieve this purpose, this invention
According to the structure of the EL panel, the back electrode is made of aluminum, the thickness of this back electrode is t, and the laminated thickness of the first insulating film, the light emitting film, and the second insulating film is T.
In this case, the film thickness ratio t/T is set to t/T≧0.5.
(作用)
この考案の考案者は、ELパネル構造を第4図
に示した構造と同様な構造とし、その構造におい
て背面電極20の膜厚tと第一絶縁膜14、発光
膜16及び第二絶縁膜18の積層厚Tとを種々の
値に設定して膜厚比t/Tと破壊穴24及び26
の直径比d2/d1との関係を調べる実験を行つた。(Function) The inventor of this device created an EL panel structure similar to the structure shown in FIG. By setting the laminated thickness T of the insulating film 18 to various values, the film thickness ratio t/T and the breakdown holes 24 and 26 are determined.
An experiment was conducted to investigate the relationship between the diameter ratio d 2 /d 1 .
第2図はこの実験結果を説明するための図で、
横軸に膜厚比t/T及び縦軸に直径比d2/d1を取
つて示してある。 Figure 2 is a diagram to explain the results of this experiment.
The horizontal axis shows the film thickness ratio t/T, and the vertical axis shows the diameter ratio d 2 /d 1 .
この実験結果からも理解出来るように、膜厚比
が約0.5より小さいと直径比が1よりも大きくな
つており、膜厚比が0.5の辺りで直径比が1とな
つており、さらに、膜厚比が0.5よりも大きな値
となるに従つて直径比が1より順次に小さくなつ
ていくのが分る。 As can be understood from this experimental result, when the film thickness ratio is smaller than about 0.5, the diameter ratio becomes larger than 1, and when the film thickness ratio is around 0.5, the diameter ratio becomes 1. It can be seen that as the thickness ratio becomes larger than 0.5, the diameter ratio becomes smaller than 1.
従つて、膜厚比t/Tをt/T≧0.5のように
設定しておけば、交流電圧印加によつて背面電極
に発生する恐れのある破壊穴の直径d2を第一絶縁
膜、発光膜及び第2絶縁膜の積層に発生する破壊
穴の直径d1よりも小さく抑制することが出来る。
これがため、例えば1mm当り10本程度の背面電極
が設けられている高精細ELパネルの場合、融点
の低いアルミニウムの背面電極に破壊穴が形成さ
れても完全に断線してしまう恐れはない。また、
アルミニウムは低抵抗材料であるので、背面電極
の両端間の抵抗差は著しく小さく、従つて、背面
電極に駆動電圧を印加したときに、背面電極の末
端部において、表示輝度ムラを起こすような電圧
降下を生じる恐れがない。また、背面電極をアル
ミニウム1種類の材料で形成しているので、背面
電極の形成工程が簡単である。 Therefore, by setting the film thickness ratio t/T to be t/T≧0.5, the diameter d2 of a breakdown hole that may occur in the back electrode due to the application of an AC voltage can be made smaller than the diameter d1 of a breakdown hole that may occur in the stack of the first insulating film, the light-emitting film, and the second insulating film.
For this reason, in the case of a high-definition EL panel having about 10 rear electrodes per mm, even if a destruction hole is formed in the rear electrode made of aluminum, which has a low melting point, there is no risk of a complete disconnection.
Since aluminum is a low resistance material, the difference in resistance between both ends of the rear electrode is extremely small, and therefore there is no risk of a voltage drop at the ends of the rear electrode causing uneven display brightness when a drive voltage is applied to the rear electrode. In addition, since the rear electrode is made of only one material, aluminum, the process of forming the rear electrode is simple.
(実施例)
以下、図面を参照してこの考案のELパネルの
実施例につき説明する。尚、図はこの考案が理解
出来る程度に概略的に示したものであり、従つ
て、各構成成分の寸法、形状、材質及び配置関係
は以下の図示例の説明にのみ限定されるものでは
ない。又、これら図において、第4図〜第6図に
示した構成部分と実質的に同一の構成部分につい
ては同一の符号を付して示し、その詳細な説明を
省略する。(Example) Examples of the EL panel of this invention will be described below with reference to the drawings. Note that the drawings are shown schematically to the extent that this invention can be understood, and therefore, the dimensions, shapes, materials, and arrangement relationships of each component are not limited to the explanations of the illustrated examples below. . Further, in these figures, components that are substantially the same as those shown in FIGS. 4 to 6 are denoted by the same reference numerals, and detailed explanation thereof will be omitted.
第1図はこの考案のELパネル構造に交流電圧
を印加したときに発生した破壊穴の状態を説明す
るための要部断面図である。尚、断面を示すハツ
チング等は省略してある。 FIG. 1 is a cross-sectional view of a main part of the EL panel structure for explaining the state of the fracture holes that occur when an alternating current voltage is applied to the EL panel structure of this invention. Note that hatching and the like indicating the cross section are omitted.
この実施例に示すELパネルでは、既に説明し
た通り、アルミニウムから成る背面電極20の厚
みをtとし及び第一絶縁膜14、発光膜16及び
第二絶縁膜18の積層厚をTとしたとき、膜厚比
t/Tをt/T≧0.5と設定し、積層厚Tに対す
る背面電極の厚みtを従来の厚みよりも厚くして
ある。 In the EL panel shown in this example, as already explained, when the thickness of the back electrode 20 made of aluminum is t, and the laminated thickness of the first insulating film 14, the light emitting film 16, and the second insulating film 18 is T, The film thickness ratio t/T is set to t/T≧0.5, and the thickness t of the back electrode relative to the lamination thickness T is made larger than the conventional thickness.
このような構造のELパネルの透明電極12と
背面電極20との間に交流電圧を継続的に印加し
て、ELパネルを発光動作させる。この時、既に
説明したような種々の欠陥があると、それぞれ直
線状に形成されている透明電極12と背面電極2
0とのほぼ直交している交点において破壊穴24
及び26が発生する。この場合、背面電極20の
破壊穴26の直径d2は破壊穴24の直径d1よりも
小さく、しかも、背面電極20の破壊穴26の近
傍が盛り上つている。これは破壊時に瞬時の放電
により第一絶縁膜14、発光膜16及び第二絶縁
膜18が発熱気化すると同時に、背面電極20も
発熱して中心部が気化し、この気化の時、背面電
極20の厚みが厚いので気化量が多くまた周囲の
溶解部分も少ないので、第一絶縁膜14、発光膜
16及び第二絶縁膜18の気化によるガス圧によ
つて背面電極20の溶解部分が押し上げられ、よ
つて破壊穴近傍が盛り上るものと推測される。 An AC voltage is continuously applied between the transparent electrode 12 and the back electrode 20 of the EL panel having such a structure to cause the EL panel to emit light. At this time, if there are various defects as already explained, the transparent electrode 12 and the back electrode 2, which are formed in a straight line,
The fracture hole 24 is located at the intersection that is almost perpendicular to 0.
and 26 occur. In this case, the diameter d 2 of the fracture hole 26 of the back electrode 20 is smaller than the diameter d 1 of the fracture hole 24, and the vicinity of the fracture hole 26 of the back electrode 20 is raised. This is because the first insulating film 14, the light-emitting film 16, and the second insulating film 18 are heated and vaporized by an instantaneous discharge at the time of breakdown, and at the same time, the back electrode 20 also generates heat and its center is vaporized. Since the thickness of the back electrode 20 is thick, the amount of vaporization is large, and the surrounding melted portion is small, so the melted portion of the back electrode 20 is pushed up by the gas pressure caused by the vaporization of the first insulating film 14, the light emitting film 16, and the second insulating film 18. Therefore, it is presumed that the area near the fracture hole swells.
しかしながら、第3図の要部斜視図に示すよう
に、破壊穴24(点線で示す。)は大きいが、こ
の破壊穴26(実線で示す。)の直径d2は背面電
極20と透明電極12の交差点での最大幅よりも
小さいので、この破壊穴26が直線状の背面電極
20の幅方向の断線を来す恐れはない。従つて、
例えば1mm当り10本程度場合によつてそれ以上の
高精細なELマトリクス表示パネルにおいても、
このパネルの駆動を信頼性高く行うことが出来
る。 However, as shown in the main part perspective view of FIG. 3, although the fracture hole 24 (indicated by a dotted line) is large, the diameter d 2 of this fracture hole 26 (indicated by a solid line) Since the width of the broken hole 26 is smaller than the maximum width at the intersection, there is no fear that the broken hole 26 will break the straight back electrode 20 in the width direction. Therefore,
For example, even in high-definition EL matrix display panels with about 10 lines per 1 mm or more in some cases,
This panel can be driven with high reliability.
尚、上述した実施例において、破壊穴の大きさ
を直径で説明したが、破壊穴の形状が円形でない
場合にはこの直径は破壊穴の最大幅のことを意味
するものとする。 In the above-mentioned embodiments, the size of the fractured hole was explained in terms of the diameter, but if the shape of the fractured hole is not circular, this diameter means the maximum width of the fractured hole.
また、上述した実施例では、ELパネルの構成
部分を特定の材料で形成した例で説明したが、こ
の考案はこれら材料には何等特定されるものでは
なく、ELパネルの構成に用いられる他の一般の
材料で形成した場合にも適用出来る。 Furthermore, in the above-mentioned embodiments, the constituent parts of the EL panel were explained as examples made of specific materials, but this invention is not limited to these materials in any way, but may be applied to other materials used in the construction of the EL panel. It can also be applied when formed from general materials.
(考案の効果)
上述した説明からも明らかなように、この考案
のELパネルによれば、膜厚比t/Tを従来とは
異なるt/T≧0.5のよう新しい領域に設定した
ので、背面電極の破壊穴の大きさが第一絶縁膜、
発光膜及び第二絶縁膜に形成される破壊穴よりも
小さくなり、従つて、10本/1mm程度又はそれ以
下の高精細なELパネルであつても、融点の低い
アルミニウムの背面電極が破壊穴で断線する恐れ
がない。また、アルミニウムは低抵抗材料である
ので、背面電極の両端間の抵抗差は著しく小さ
く、従つて、背面電極に駆動電圧を印加したとき
に、背面電極の末端部において、表示輝度ムラを
起こすような電圧降下を生じる恐れがない。従つ
て、この考案のELパネルでは良好なマトリクス
表示を行うことが出来る。また、背面電極をアル
ミニウム1種類の材料で形成しているので、背面
電極の形成工程が簡単である。(Effects of the invention) As is clear from the above explanation, according to the EL panel of this invention, the film thickness ratio t/T is set in a new region such as t/T≧0.5, which is different from the conventional one, so that the back The size of the fracture hole in the electrode is the first insulating film,
The holes are smaller than those formed in the light-emitting film and the second insulating film. Therefore, even in a high-definition EL panel with about 10 lines/1 mm or less, the back electrode made of aluminum, which has a low melting point, will prevent the holes from breaking. There is no risk of disconnection. In addition, since aluminum is a low resistance material, the difference in resistance between both ends of the back electrode is extremely small. Therefore, when a driving voltage is applied to the back electrode, uneven display brightness may occur at the end of the back electrode. There is no risk of significant voltage drop. Therefore, the EL panel of this invention can perform a good matrix display. Furthermore, since the back electrode is made of one type of material, aluminum, the process for forming the back electrode is simple.
第1図はこの考案のELパネルの一実施例を説
明するための、破壊穴が発生した状態での要部断
面図、第2図はこの考案のELパネルの説明に供
する背面電極の厚みと第一絶縁膜、発光膜及び第
二絶縁膜との間の膜厚比と、破壊穴の直径比との
関係を示す説明図、第3図はこの考案のELパネ
ルの動作を説明するための要部斜視図、第4図は
この考案及び従来のELパネルの説明に供するEL
発光素子の要部断面図、第5図は従来の破壊穴の
状態を説明するためのELパネル要部断面図、第
6図は従来のELパネルの動作を説明するための
要部斜視図である。
10……ガラス基板、12……透明電極、14
……第一絶縁膜、16……発光膜、18……第二
絶縁膜、20……背面電極、22……目視方向、
24,26……破壊穴。
Figure 1 is a cross-sectional view of the main part in a state where a fracture hole has occurred to explain an embodiment of the EL panel of this invention, and Figure 2 shows the thickness of the back electrode to explain the EL panel of this invention. An explanatory diagram showing the relationship between the film thickness ratio of the first insulating film, the light-emitting film, and the second insulating film and the diameter ratio of the fracture hole, and Figure 3 is a diagram for explaining the operation of the EL panel of this invention. A perspective view of the main part, Figure 4 is an EL panel used to explain this invention and the conventional EL panel.
Figure 5 is a cross-sectional view of the main part of a light emitting element, Figure 5 is a cross-sectional view of the main part of an EL panel to explain the state of the conventional fracture hole, and Figure 6 is a perspective view of the main part to explain the operation of the conventional EL panel. be. 10...Glass substrate, 12...Transparent electrode, 14
...First insulating film, 16... Luminescent film, 18... Second insulating film, 20... Back electrode, 22... Viewing direction,
24, 26... Destruction hole.
Claims (1)
に設けられた第一及び第二絶縁膜と、第一絶縁膜
の外側に設けられた透明電極と、第二絶縁膜の外
側に設けられた背面電極とを含む交流形薄膜2重
絶縁構造のエレクトロルミネツセンスパネルにお
いて、 前記背面電極はアルミニウムから成つており、
かつ、該背面電極の厚みをtとし及び前記第一絶
縁膜、発光膜及び第二絶縁膜の積層厚をTとした
とき、t/T≧0.5とした ことを特徴とするエレクトロルミネツセンスパネ
ル。[Claims for Utility Model Registration] A light-emitting film, first and second insulating films provided to sandwich the light-emitting film from both sides, a transparent electrode provided on the outside of the first insulating film, and a second insulating film. In an electroluminescent panel having an AC type thin film double insulation structure including a back electrode provided on the outside of the membrane, the back electrode is made of aluminum,
and an electroluminescent panel characterized in that t/T≧0.5, where t is the thickness of the back electrode and T is the laminated thickness of the first insulating film, the light emitting film, and the second insulating film. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1986095583U JPH0524155Y2 (en) | 1986-06-23 | 1986-06-23 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1986095583U JPH0524155Y2 (en) | 1986-06-23 | 1986-06-23 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS632396U JPS632396U (en) | 1988-01-08 |
| JPH0524155Y2 true JPH0524155Y2 (en) | 1993-06-18 |
Family
ID=30960288
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1986095583U Expired - Lifetime JPH0524155Y2 (en) | 1986-06-23 | 1986-06-23 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0524155Y2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS59126793U (en) * | 1983-02-15 | 1984-08-25 | 株式会社シマノ | Bicycle speed control device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61284093A (en) * | 1985-06-07 | 1986-12-15 | シャープ株式会社 | Thin film electric field light emitting element |
-
1986
- 1986-06-23 JP JP1986095583U patent/JPH0524155Y2/ja not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS632396U (en) | 1988-01-08 |
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