JPS63200433A - Plasma display panel - Google Patents

Plasma display panel

Info

Publication number
JPS63200433A
JPS63200433A JP62033957A JP3395787A JPS63200433A JP S63200433 A JPS63200433 A JP S63200433A JP 62033957 A JP62033957 A JP 62033957A JP 3395787 A JP3395787 A JP 3395787A JP S63200433 A JPS63200433 A JP S63200433A
Authority
JP
Japan
Prior art keywords
group
partition walls
plasma display
display panel
insulator
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
JP62033957A
Other languages
Japanese (ja)
Other versions
JPH0616377B2 (en
Inventor
Osamu Taneda
修 種田
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.)
NEC Corp
Original Assignee
NEC Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Corp filed Critical NEC Corp
Priority to JP62033957A priority Critical patent/JPH0616377B2/en
Publication of JPS63200433A publication Critical patent/JPS63200433A/en
Publication of JPH0616377B2 publication Critical patent/JPH0616377B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To make it possible to obtain a plasma display panel with a larger range of operating voltage suitable for the face selection drive method by making a layer of a group of insulating matter partition walls between scanning electrodes with a strong cross talk thicker than a layer of a group of insulating matter partition walls between data electrodes with a week cross talk. CONSTITUTION:A layer of a group of insulating matter partition walls 7 is formed to be 75mum thick, and a layer of a group of insulating matter partition walls 8 is formed to be 25mum thick to have different thickness from each other. As an example of forming them, the group of insulating matter partition walls 8 may be formed to have thickness of 25mum by screen printing once and the insulating matter partition walls 8 to be 75mum thick by screen printing three times easily. By making the insulating matter partition walls 7 thicker for scanning directions with a stronger cross talk and the insulating matter partition walls 8 thinner between data electrodes for which cross talk is weaker, a plasma display panel with reduced cross talk can be realized. Balance of thickness can be changed depending on the voltage to be applied.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はプラズマディスプレイパネル、特にプラズマデ
ィスプレイパネルの動作電圧マージンを改善するための
絶縁体隔壁の構造に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a plasma display panel, and more particularly to a structure of an insulator barrier rib for improving the operating voltage margin of a plasma display panel.

〔従来の技術〕[Conventional technology]

従来よりACリフレッシュ形プラズマディスプレイパネ
ルに於いては、絶縁体隔壁の構造に独自のものがあり、
この絶縁体隔壁は隣接セル間のクロストークを防止する
のと同時に、放電ギャップを一定に保つためのスペーサ
として利用されている。従来のプラズマディスプレイパ
ネルの絶縁体隔壁について第3図を用いて説明する。
Conventionally, AC refresh type plasma display panels have a unique structure of insulator partition walls.
This insulator barrier rib is used as a spacer to prevent crosstalk between adjacent cells and to maintain a constant discharge gap. The insulator partition wall of a conventional plasma display panel will be explained with reference to FIG.

第3図は従来のプラズマディスプレイパネルの断面図で
あり、1は前面基板、2は後面基板、3は前面基板1の
内面上に形成されたSnO□等の透明電極、4は後面基
板2の内面上に形成された例えば銀電極である。透明電
極3は誘電体膜5によって被覆され、銀電極4は誘電体
膜6によって被覆されている。さらに誘電体膜5の上に
は、透明電極3と直交するように絶縁体隔壁7が形成さ
れ、誘電体膜6の上には銀電極4と直交するように絶縁
体隔壁8が形成されている。絶縁体隔壁7が銀電極4の
間隙に位置し、絶縁体隔壁8が透明電極3の間隙に位置
するように前面基板1と後面基板2とを相対向させ、封
止材9によって気密封止し、パネル内部を真空に排気し
た上でNe等の希ガスが封入されている。後述する理由
仲より、絶縁体隔壁7と8とは、はぼ同じ厚さ、例えば
50μmの厚さで形成されている。
FIG. 3 is a cross-sectional view of a conventional plasma display panel, in which 1 is a front substrate, 2 is a rear substrate, 3 is a transparent electrode such as SnO□ formed on the inner surface of the front substrate 1, and 4 is a transparent electrode of the rear substrate 2. For example, a silver electrode formed on the inner surface. The transparent electrode 3 is covered with a dielectric film 5, and the silver electrode 4 is covered with a dielectric film 6. Furthermore, an insulator partition 7 is formed on the dielectric film 5 so as to be perpendicular to the transparent electrode 3 , and an insulator partition 8 is formed on the dielectric film 6 so as to be perpendicular to the silver electrode 4 . There is. The front substrate 1 and the rear substrate 2 are opposed to each other so that the insulating partition wall 7 is located in the gap between the silver electrodes 4 and the insulating partition wall 8 is located in the gap between the transparent electrodes 3, and hermetically sealed with the sealing material 9. However, the inside of the panel is evacuated and then a rare gas such as Ne is sealed. For reasons described later, the insulator partition walls 7 and 8 are formed to have approximately the same thickness, for example, 50 μm.

次に、絶縁体隔壁7と8とが同じ層厚で形成される理由
について述べる。第4図はプラズマディスプレイパネル
の電極を模式的に示した図であり、第5図はかかる電極
に印加される電圧波形を示した図である。第4図におけ
る3−1,3−2,3−3,4−1,4−2,4−3は
第3図に於ける透明電極3および銀電極4に番号1〜3
を付したものである。また第5図は電極3−1.3−2
.3−3および4−1.4−2.4−3に印加される電
圧波形例を示すものである。第5図に於いて、4−1.
4−2.4−3は走査用電圧波形であり、3−1.3−
2.3−3は走査電圧波形に対応して印加されるデータ
電圧波形である。
Next, the reason why insulator partition walls 7 and 8 are formed with the same layer thickness will be described. FIG. 4 is a diagram schematically showing electrodes of a plasma display panel, and FIG. 5 is a diagram showing voltage waveforms applied to such electrodes. 3-1, 3-2, 3-3, 4-1, 4-2, 4-3 in FIG. 4 are numbers 1 to 3 for the transparent electrode 3 and silver electrode 4 in FIG.
. In addition, Fig. 5 shows the electrode 3-1.3-2.
.. 3-3 and 4-1.4-2.4-3 are shown as example voltage waveforms. In Figure 5, 4-1.
4-2.4-3 is the voltage waveform for scanning, and 3-1.3-
2.3-3 is a data voltage waveform applied corresponding to the scanning voltage waveform.

選択時には、Voなる波高値を有する走査電圧パルスと
逆位相のやはりVOなる波高値を有する電圧パルスがデ
ータ電圧として印加される。Voは通常150Vに設定
されている。今、Tなるタイミングで考えると、第4図
に示す電極4−2と電極3−2との交点の放電セル(4
−2,:3−2)が選択され放電発光する。ところで、
放電セル(4−1,3−2)、(4−2,3−1)、(
4−2,3−3)および(4−3,3−2)は半選択状
態にあり、かつ放電状態にある隣接セルには150V+
150V=300Vに相当する電界の変化が与えられて
いる為、隣接セル間のクロストークが大きな問題となる
。従って、このセル間のクロストークを切る為に絶縁体
間隔が必要となり、しかもX方向およびy方向に対して
等しくクロストークを遮断するため絶縁体隔壁7および
8を等しい障壁の高さに形成する必要がある。
At the time of selection, a voltage pulse having a peak value of VO and having a phase opposite to the scanning voltage pulse having a peak value of Vo is applied as a data voltage. Vo is normally set to 150V. Now, considering the timing T, the discharge cell (4) at the intersection of electrode 4-2 and electrode 3-2 shown in FIG.
-2, :3-2) is selected and discharge light is emitted. by the way,
Discharge cells (4-1, 3-2), (4-2, 3-1), (
4-2, 3-3) and (4-3, 3-2) are in the half-selected state, and the adjacent cells in the discharge state are supplied with 150V+.
Since a change in the electric field corresponding to 150V=300V is given, crosstalk between adjacent cells becomes a big problem. Therefore, insulator spacing is required to cut this crosstalk between cells, and insulator partition walls 7 and 8 are formed to have equal barrier heights in order to block crosstalk equally in the X and Y directions. There is a need.

しかるに最近、プラズマディスプレイは高精細でCRT
に匹敵する大表示容量を有する製品の需要が急増してお
り、かかるディスプレイの消費電力を軽減する為に、走
査用電極には180■のパルス電圧を印加し、データ用
電極には30Vのパルス電圧をデータの有無に対応して
、その極性を制御して印加する所謂フェースセレクショ
ン駆動方式が実用化されている。
However, recently, plasma displays are high-definition and CRT
The demand for products with a large display capacity comparable to that of 2000 is rapidly increasing, and in order to reduce the power consumption of such displays, a pulse voltage of 180V is applied to the scanning electrodes, and a pulse voltage of 30V is applied to the data electrodes. A so-called face selection driving method has been put into practical use in which a voltage is applied while controlling its polarity depending on the presence or absence of data.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところが、前述したフェースセレクション駆動により、
セル間ピッチが0.4mm以下の高精細な第3図に示す
従来のプラズマディスプレイパネルを駆動した場合、走
査方向のクロストークが問題となることが明らかとなっ
た。
However, due to the face selection drive mentioned above,
It has become clear that crosstalk in the scanning direction becomes a problem when driving a high-definition conventional plasma display panel shown in FIG. 3 with an inter-cell pitch of 0.4 mm or less.

本発明は、従来のプラズマディスプレイパネルの絶縁体
隔壁の構造を変えることにより、フェースセレクション
駆動方式による走査方向クロストークの問題を解決する
ものである。
The present invention solves the problem of crosstalk in the scanning direction caused by the face selection drive method by changing the structure of the insulator partition of the conventional plasma display panel.

〔問題点を解決するための手段〕[Means for solving problems]

本発明のプラズマディスプレイパネルは、前面基板上に
誘電体膜にて被覆した互いに平行な透明電極群を形成し
、さらに、この透明電極群と直交するように誘電体膜上
に第1の絶縁体隔壁群を形成し、一方、後面基板上に誘
電体膜にて被覆した互いに平行な電極群を形成し、さら
にこの電極群と直交するように誘電体膜上に第2−の絶
縁体隔壁群を形成し、前面基板と後面基板とを透明電極
群と後面基板側の電極群とが互いに直交し、かつ第1の
絶縁体隔壁群が後面基板側の電極群の間隙に配置され、
第2の絶縁体隔壁群が前面基板側の透明電極群の間隙に
配置されるよう相対向させ、第1の絶縁体隔壁群の厚さ
と、第2の絶縁体隔壁群の厚さによって放電ギャップが
決定されるよう気密封止し、内部に放電可能な希ガスを
封入して成るプラズマディスプレイパネルにおいて、第
1の絶縁体隔壁群の厚みと、第2の絶縁体隔壁群の厚み
とを互いに異なる厚みに形成した構造を有する。
In the plasma display panel of the present invention, a group of parallel transparent electrodes covered with a dielectric film is formed on a front substrate, and a first insulator is further formed on the dielectric film so as to be perpendicular to the transparent electrode group. On the other hand, a group of parallel electrodes covered with a dielectric film is formed on the rear substrate, and a second group of insulating partition walls is formed on the dielectric film perpendicularly to the electrode group. forming a front substrate and a rear substrate, the transparent electrode group and the electrode group on the rear substrate side are perpendicular to each other, and the first insulator partition group is arranged in the gap between the electrode group on the rear substrate side,
The second insulator barrier rib group is arranged opposite to each other so as to be disposed in the gap between the transparent electrode groups on the front substrate side, and the discharge gap is determined by the thickness of the first insulator barrier rib group and the thickness of the second insulator barrier rib group. In a plasma display panel that is hermetically sealed and has a dischargeable rare gas filled inside so that the It has a structure formed with different thicknesses.

〔実施例〕〔Example〕

次に、本発明について図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.

第1図は本発明の一実施例の断面図である。参照数字1
〜6および9は第3図に示した従来のプラズマディスプ
レイと同様であるので説明は省略し、第3図と異なる絶
縁体隔壁群7および8について説明する。従来のプラズ
マディスプレイパネルを示す第3図においては、絶縁体
隔壁群7および8が同じ層厚〜50μmに形成されてい
るのに対し、本発明の一実施例を示す第1図においては
、絶縁体隔壁群7の層厚を75μmに、絶縁体隔壁群8
の層厚を25μmに各々の層厚を変えて形成する。形成
方法は、例えば、絶縁体隔壁群8を1回のスクリーン印
刷により25μmの層厚に形成し、一方、絶縁体隔壁群
7を3回のスクリーン印刷により所望の75μmの層厚
に容易に形成することができる。
FIG. 1 is a sectional view of an embodiment of the present invention. Reference number 1
6 and 9 are the same as those of the conventional plasma display shown in FIG. 3, so their explanation will be omitted, and the insulator barrier rib groups 7 and 8, which are different from those in FIG. 3, will be explained. In FIG. 3 showing a conventional plasma display panel, insulator partition groups 7 and 8 are formed to have the same layer thickness of 50 μm, whereas in FIG. The layer thickness of the body partition group 7 is 75 μm, and the layer thickness of the insulator partition group 8 is 75 μm.
The layer thickness of each layer is changed to 25 μm. For example, the insulator barrier rib group 8 is formed to a layer thickness of 25 μm by one screen printing, while the insulator barrier rib group 7 is easily formed to a desired layer thickness of 75 μm by three times of screen printing. can do.

次に、第1図に示すプラズマディスプレイパネルの動作
を第2図に示すフェースセレクション駆動方式のパルス
波形を用いて説明する。今、Tなるタイミングで考える
と、第4図に示す電極4−2と電極3−2との交点の放
電セル(4−2,3−2)に180+30=210Vの
電圧変化が与えられ、放電発光する。放電セル(4−1
,3−2)、(4−2,3−1)、(4−2,3−3)
および(4−3,3−2)は半選択状態にあるが、放電
セル(4−1,3−2>および(4−3,3−2)には
高々30Vの電圧変化が与えられるのみであり、また放
電セル(4−2,3−1)および(4−2,3−3)に
は180−30=150Vの電圧変化が与えられ、従来
の駆動波形第5図の場合と同様である。しかるに隣接す
る選択放電セル(4−2,3−2)には、従来の駆動波
形の場合の150+150=300Vに対して低い電圧
変化、180+30=210Vの電圧変化が与えている
為、隣接セル間のクロストークはかなり低減されること
になる。ところが、第2図に示す新駆動方式においては
、従来と異なるクロストークが存在することが明らかと
なった。
Next, the operation of the plasma display panel shown in FIG. 1 will be explained using the pulse waveform of the face selection driving method shown in FIG. 2. Now, considering the timing T, a voltage change of 180+30=210V is applied to the discharge cell (4-2, 3-2) at the intersection of electrode 4-2 and electrode 3-2 shown in FIG. Emits light. Discharge cell (4-1
, 3-2), (4-2, 3-1), (4-2, 3-3)
and (4-3, 3-2) are in a half-selected state, but a voltage change of at most 30 V is applied to discharge cells (4-1, 3-2> and (4-3, 3-2)) Also, a voltage change of 180-30=150V is given to the discharge cells (4-2, 3-1) and (4-2, 3-3), and the same as in the case of the conventional drive waveform shown in FIG. However, since the adjacent selective discharge cells (4-2, 3-2) are given a voltage change of 180+30=210V, which is lower than the 150+150=300V in the case of the conventional drive waveform, Crosstalk between adjacent cells will be considerably reduced. However, it has become clear that in the new drive method shown in FIG. 2, crosstalk different from the conventional one exists.

今、タイミングTからタイミングT+1に移る過渡期を
考えると、従来の場合には走査用電格4−2と4−3の
間には150+150=300Vの電圧変化が与えられ
るのに対し、第2図に示す駆動の場合には180+18
0=360Vの電圧変化が与えられる為、走査方向への
電荷結合が非常に強くなり、従って、走査方向に対する
セル間クロストークが問題となる。以上説明したセル間
スロストークの機構を解明することにより、本発明によ
るプラズマディスプレイパネルに於いては、クロストー
クの強い走査方向に対しては、絶縁体隔壁7の層厚を厚
くし、クロストークの弱いデータ電極間の絶縁体隔壁8
の層厚を薄くすることにより、クロストークの少ないプ
ラズマディスプレイパネルを実現することができた。
Now, considering the transition period from timing T to timing T+1, in the conventional case, a voltage change of 150 + 150 = 300V is applied between scanning voltages 4-2 and 4-3, whereas In the case of the drive shown in the figure, 180+18
Since a voltage change of 0=360V is applied, charge coupling in the scanning direction becomes very strong, and therefore inter-cell crosstalk in the scanning direction becomes a problem. By elucidating the mechanism of inter-cell crosstalk explained above, in the plasma display panel according to the present invention, in the scanning direction where crosstalk is strong, the layer thickness of the insulator partition 7 is increased to reduce crosstalk. Insulator partition between weak data electrodes 8
By reducing the layer thickness, we were able to create a plasma display panel with less crosstalk.

また、実施例においては、走査電極間絶縁体隔壁群の層
厚を75μm、データ電極間絶縁体隔壁群の層厚を25
μmとしたが、印加する電圧の大小により、適当に層厚
のバランスを変えることができる。
In addition, in the example, the layer thickness of the insulator barrier rib group between scanning electrodes is 75 μm, and the layer thickness of the insulator barrier rib group between data electrodes is 25 μm.
Although the thickness is .mu.m, the balance of the layer thickness can be changed appropriately by changing the magnitude of the applied voltage.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、クロストークの強い走査
電極間の絶縁体隔壁群の層厚を、クロストークの弱いデ
ータ電極間の絶縁体隔壁群の層厚より°厚くすることに
より、フェースセレクション駆動方式に適した動作電圧
範囲の広いプラズマディスプレイパネルを提供すること
ができる。
As explained above, the present invention achieves face selection by making the layer thickness of the insulator barrier rib group between scanning electrodes with strong crosstalk thicker than the layer thickness of the insulator barrier rib group between data electrodes with weak crosstalk. A plasma display panel with a wide operating voltage range suitable for the driving method can be provided.

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

第1図は本発明のプラズマディスプレイパネルの一実施
例を示す断面図、第2図は本発明のプラズマディスプレ
イパネルを駆動する駆動パルス例を示す図、第3図は従
来のプラズマディスプレイを示す断面図、第4図はプラ
ズマディスプレイパネルの電極を模式的に示した図、第
5図は従来の駆動パルス例を示す図である。 1・・・前面基板、2・・・後面基板、3・・・透明電
極(データ用電極)、4・・・後面電極(走査用電極)
、5.6・・・誘電体膜、7,8・・・絶縁体隔壁、9
・・・封止材、4−1.4−2.4−3・・・走査用電
極、3−1.3−2.3−3・・・データ用電極。 (トープ 憶 第 21!r 茅 4 図
FIG. 1 is a cross-sectional view showing an embodiment of the plasma display panel of the present invention, FIG. 2 is a view showing an example of a driving pulse for driving the plasma display panel of the present invention, and FIG. 3 is a cross-sectional view showing a conventional plasma display. 4 are diagrams schematically showing electrodes of a plasma display panel, and FIG. 5 is a diagram showing an example of a conventional drive pulse. 1... Front substrate, 2... Rear substrate, 3... Transparent electrode (data electrode), 4... Back electrode (scanning electrode)
, 5.6... Dielectric film, 7, 8... Insulator partition, 9
...Sealing material, 4-1.4-2.4-3...Scanning electrode, 3-1.3-2.3-3...Data electrode. (Top Memory Day 21! R Kaya 4 Figure

Claims (1)

【特許請求の範囲】[Claims]  基板上に互いに平行な第1の電極群を形成し、該第1
の電極群を誘電体膜にて被覆し、さらに前記第1の電極
群と直交するように前記誘電体膜上に形成した第1の絶
縁体隔壁群を有する前面基板と、基板上に互いに平行な
第2の電極群を形成し、該第2の電極群を誘電体膜にて
被覆し、さらに前記第2の電極群と直交するように前記
誘電体膜上に形成した第2の絶縁体隔壁群を有する後面
基板とを、前記第1の電極群と前記第2の電極群とが互
いに直交し、かつ前記第1の絶縁体隔壁群が前記第2の
電極群の間に配置され、前記第2の絶縁体隔壁群が前記
第1の電極群の間に配置されるよう相対向させ、前記第
1の絶縁体隔壁群の厚さと、前記第2の絶縁体隔壁群の
厚さによって放電ギャップが決定されるように気密封止
し、内部に放電可能な希ガスを封入して成るプラズマデ
ィスプレイパネルにおいて、前記第1の絶縁体隔壁群と
前記第2の絶縁体隔壁群とを互いに異なる厚みに形成し
たことを特徴とするプラズマディスプレイパネル。
forming a first electrode group parallel to each other on the substrate;
a front substrate having a first insulating barrier rib group formed on the dielectric film so as to be perpendicular to the first electrode group; forming a second electrode group, covering the second electrode group with a dielectric film, and further forming a second insulator on the dielectric film so as to be perpendicular to the second electrode group. a rear substrate having a group of partition walls, the first electrode group and the second electrode group are orthogonal to each other, and the first insulator partition group is arranged between the second electrode group; The second insulator barrier rib group is disposed between the first electrode group and faces each other, and the thickness of the first insulator barrier rib group and the second insulator barrier rib group are In a plasma display panel that is hermetically sealed so that a discharge gap is determined and a dischargeable rare gas is filled inside, the first insulator barrier rib group and the second insulator barrier rib group are connected to each other. A plasma display panel characterized by being formed with different thicknesses.
JP62033957A 1987-02-16 1987-02-16 Plasma display panel Expired - Lifetime JPH0616377B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62033957A JPH0616377B2 (en) 1987-02-16 1987-02-16 Plasma display panel

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62033957A JPH0616377B2 (en) 1987-02-16 1987-02-16 Plasma display panel

Publications (2)

Publication Number Publication Date
JPS63200433A true JPS63200433A (en) 1988-08-18
JPH0616377B2 JPH0616377B2 (en) 1994-03-02

Family

ID=12400968

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62033957A Expired - Lifetime JPH0616377B2 (en) 1987-02-16 1987-02-16 Plasma display panel

Country Status (1)

Country Link
JP (1) JPH0616377B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05121004A (en) * 1991-10-25 1993-05-18 Nec Corp Plasma display panel

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05121004A (en) * 1991-10-25 1993-05-18 Nec Corp Plasma display panel

Also Published As

Publication number Publication date
JPH0616377B2 (en) 1994-03-02

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