JPH0346941B2 - - Google Patents

Info

Publication number
JPH0346941B2
JPH0346941B2 JP59004170A JP417084A JPH0346941B2 JP H0346941 B2 JPH0346941 B2 JP H0346941B2 JP 59004170 A JP59004170 A JP 59004170A JP 417084 A JP417084 A JP 417084A JP H0346941 B2 JPH0346941 B2 JP H0346941B2
Authority
JP
Japan
Prior art keywords
electrode
discharge
enlarged
enlarged portion
circular
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.)
Expired - Lifetime
Application number
JP59004170A
Other languages
Japanese (ja)
Other versions
JPS60148035A (en
Inventor
Hiraki Uchiike
Tsutae Shinoda
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP59004170A priority Critical patent/JPS60148035A/en
Publication of JPS60148035A publication Critical patent/JPS60148035A/en
Publication of JPH0346941B2 publication Critical patent/JPH0346941B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J11/00Gas-filled discharge tubes with alternating current induction of the discharge, e.g. alternating current plasma display panels [AC-PDP]; Gas-filled discharge tubes without any main electrode inside the vessel; Gas-filled discharge tubes with at least one main electrode outside the vessel

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Gas-Filled Discharge Tubes (AREA)

Description

【発明の詳細な説明】 (a) 発明の技術分野 この発明は、面放電型ガス放電パネル、特に発
光輝度を向上したパネル構造に関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION (a) Technical Field of the Invention The present invention relates to a surface discharge type gas discharge panel, and particularly to a panel structure with improved luminance.

(b) 技術の背景 AC駆動形式のガス放電パネルの一種に面放電
型と呼ばれるパネルがある。この形式のガス放電
パネルは、ガス封入空間を挟んで対向位置した一
対の基板の内の一方の基板上にのみX電極とY電
極の両方を配設し、これら両電極の交点近傍にお
いて基板の両方向に沿つた横放電を発生させるよ
うにしたところに特徴をそなえている。しかして
かかる構成によれば、一対の基板間の間隙精度に
対する要求が著しく緩和される他、カバー用の基
板内面に紫外線励起形の螢光体を付設して表示色
の変換や多色化が容易に行えるという利点があ
る。このことから最近特に注目され、デイスプレ
イパネルへの実用化に沿つた高輝度化の研究が進
められている。
(b) Technical background One type of AC-driven gas discharge panel is a panel called a surface discharge type. In this type of gas discharge panel, both an X electrode and a Y electrode are disposed on only one of a pair of substrates located opposite to each other with a gas-filled space in between. Its unique feature is that it generates horizontal discharge along both directions. According to such a configuration, the requirement for the gap accuracy between the pair of substrates is significantly relaxed, and an ultraviolet-excited phosphor is added to the inner surface of the cover substrate, allowing for conversion of display colors and multicolor display. It has the advantage of being easy to perform. For this reason, it has recently attracted particular attention, and research is underway to increase its brightness for practical use in display panels.

(c) 従来技術と問題点 第1図および第2図は特開昭57−74940号に開
示された従来の面放電型ガス放電パネルの電極配
置の一例を示す平面図とそれの−線に沿つた
断面図である。これらの図において、1は電極支
持基板として機能する下側ガラス基板、2は横方
向に複数配列された下層のX電極、3は低融点ガ
ラス等よりなる誘電体層、4は前記X電極と直交
させて縦方向に複数配列したY電極である。前記
X電極2およびY電極4の交叉部は、符号2aと
4aで示すようにそれぞれ電極幅方向に膨大した
円形状とされガス放電部を構成する。なお、X電
極の円形膨大部2aはY電極の円形膨大部4aを
完全に包囲するように大きく設定されている。ま
た5は該Y電極をガス封入空間6と絶縁する絶縁
層で、低融点ガラス等の誘電体と酸化マグネシウ
ムとの積層体より構成される。また7は前記下側
電極支持基板構体に対向配置されてガス封入空間
6を構成するカバー用上側ガラス基板である。
(c) Prior art and problems Figures 1 and 2 are a plan view showing an example of the electrode arrangement of a conventional surface discharge type gas discharge panel disclosed in JP-A No. 57-74940, and the - line in the plan view. FIG. In these figures, 1 is a lower glass substrate that functions as an electrode support substrate, 2 is a lower layer of X electrodes arranged in a plurality of horizontal directions, 3 is a dielectric layer made of low melting point glass, etc., and 4 is the X electrode and the lower layer. A plurality of Y electrodes are arranged in the vertical direction so as to be orthogonal to each other. The intersection portions of the X electrode 2 and the Y electrode 4 are each formed into a circular shape that expands in the electrode width direction, as shown by reference numerals 2a and 4a, and constitute a gas discharge portion. Note that the circular enlarged portion 2a of the X electrode is set to be large enough to completely surround the circular enlarged portion 4a of the Y electrode. Further, 5 is an insulating layer that insulates the Y electrode from the gas-filled space 6, and is made of a laminate of a dielectric material such as low melting point glass and magnesium oxide. Reference numeral 7 denotes an upper glass substrate for a cover, which is disposed opposite to the lower electrode support substrate structure and constitutes the gas-filled space 6.

このようなパネル構成において、選択したX電
極とY電極に対しそれらの合成電圧が放電開始電
位を越えるような電圧を印加すると、交叉した両
電極における円形膨大部2a,4aのエツジ部間
に電界が発生することにより、当該電極交叉部に
放電が発生する。このX、Y電極間の放電は、各
電極面が交互にカソードとなつて陰極グローを生
じるような形で行われるが、下層X電極の円形膨
大部を上層Y電極の円形膨大部よりも大きく形成
した特徴構造によつて、下層X電極側がカソード
となつて放電する場合、上層Y電極側がカソード
となつて放電する場合のいずれにおいても略均一
な大きさの円形に近いシヤープは放電スポツトと
なる。従つて、隣接放電点間を狭くでき解像度を
向上できる(詳細は前記特開昭57−74940号を参
照)。ところがこの電極構造では、電流集中が生
じている電極エツジ部周囲は比較的高い輝度で発
光するけれども、上層のY電極4の中心部は電界
が発生しないために暗部となり、視覚的にみて中
心部の暗い放電点形態を呈する。従つて、放電部
の発光輝度が低く、デイスプレイパネルとして使
用した場合表示が見難いという欠点があつた。
In such a panel configuration, when a voltage is applied to the selected X electrode and Y electrode such that their combined voltage exceeds the discharge starting potential, an electric field is generated between the edges of the circular enlarged portions 2a and 4a of the crossed electrodes. As a result, a discharge occurs at the electrode intersection. This discharge between the X and Y electrodes occurs in such a way that each electrode surface alternately serves as a cathode, producing a cathode glow. Depending on the formed characteristic structure, a nearly circular sharp with a uniform size becomes a discharge spot in both cases when the lower layer X electrode side acts as a cathode and discharges, and when the upper layer Y electrode side acts as a cathode and discharges. . Therefore, the distance between adjacent discharge points can be narrowed and the resolution can be improved (for details, see the above-mentioned Japanese Patent Laid-Open No. 74940/1983). However, in this electrode structure, although the area around the electrode edge where current concentration occurs emits light with relatively high brightness, the center of the upper layer Y electrode 4 becomes a dark area because no electric field is generated, and visually the center It exhibits a dark discharge point morphology. Therefore, the luminance of the discharge portion is low and the display is difficult to see when used as a display panel.

(d) 発明の目的 この発明は、以上のような状況から絶縁膜を挟
んで上下に一対の電極を対向配置した形式の面放
電型ガス放電パネルの表示品質の向上を目的とす
るものであり、さらに具体的には電極構造を改良
して光輝度発光を図ろうとするものである。
(d) Purpose of the Invention In view of the above-mentioned circumstances, the present invention aims to improve the display quality of a surface discharge type gas discharge panel in which a pair of electrodes are disposed above and below to face each other with an insulating film in between. More specifically, the aim is to improve the electrode structure and achieve bright luminescence.

(e) 発明の構成 簡単に述べるとこの発明の面放電型ガス放電パ
ネルは、下層電極の円形膨大部よりも小面積の上
層電極の膨大部を、リング形状にあつてその中心
孔径を外径の0.5〜0.75の比率で形成し、この孔
の内周部においても電界を発生させて放電を起こ
させる、つまりリング形の上層電極膨大部の外周
および孔内周にそれぞれ放電を発生させて放電ス
ポツトに暗部が現れないようにしたことを特徴と
するものである。
(e) Structure of the Invention Briefly stated, in the surface discharge type gas discharge panel of the present invention, the enlarged part of the upper layer electrode has a smaller area than the circular enlarged part of the lower electrode, and the enlarged part of the upper layer electrode is formed into a ring shape, with the center hole diameter being the diameter of the outer diameter. The electrode is formed at a ratio of 0.5 to 0.75, and an electric field is generated at the inner periphery of the hole to cause a discharge. The feature is that dark areas do not appear in the spots.

(f) 発明の実施例 以下、この発明の一実施例につき図面を参照し
て詳細に説明する。
(f) Embodiment of the Invention Hereinafter, an embodiment of the invention will be described in detail with reference to the drawings.

第3図および第4図はかかる実旅例に基づくパ
ネルの電極配置を示す平面図とそれの−′線
に沿つた断面図である。このパネルに上層のY電
極の形状を除いて前記第1図,第2図とほとんど
同じ構造を有し、したがつて第3図,第4図にお
いて該Y電極以外は同一符号を付して示すととも
に詳細説明を省略する。
3 and 4 are a plan view showing the electrode arrangement of a panel based on such an actual travel example, and a sectional view thereof taken along the line -'. This panel has almost the same structure as in FIGS. 1 and 2 above, except for the shape of the Y electrode on the upper layer, so in FIGS. The detailed explanation will be omitted.

すなわち、上層のY電極8は、両図に示すよう
に円形膨大部8aの中心が穿孔されている。
That is, in the upper layer Y electrode 8, as shown in both figures, the center of the circular enlarged portion 8a is perforated.

このように上層電極の膨大部8aをリング形状
にすると、その膨大部外周および孔内周部に同時
に放電を発生できる。すなわち、上層電極と下層
電極との間に点火電圧を越える電圧を印加した
時、電極間に生じる電界は当該リング形膨大部8
aの外周エツジ部および内周エツジ部に集中し、
言い換えればこの部分に電気力線が発生するた
め、このリング形膨大部の内、外周部に同時に放
電が発生する。これらの放電は上層電極上の誘電
体層表面に蓄積される壁電荷等の作用によつて該
電極膨大部の各エツジ部から外、内に向けて広が
り、結果的に中心に暗部のない略円形の放電発光
パターンとなる。
When the enlarged portion 8a of the upper layer electrode is formed into a ring shape in this manner, discharge can be generated at the outer circumference of the enlarged portion and the inner circumference of the hole simultaneously. That is, when a voltage exceeding the ignition voltage is applied between the upper layer electrode and the lower layer electrode, the electric field generated between the electrodes is
Concentrates on the outer edge and inner edge of a,
In other words, since electric lines of force are generated in this portion, electric discharge occurs simultaneously in the inner and outer peripheral portions of this ring-shaped enlarged portion. These discharges spread outward and inward from each edge of the electrode's enlarged part due to the action of wall charges accumulated on the surface of the dielectric layer on the upper electrode, resulting in a nearly flat area with no dark area at the center. This results in a circular discharge light emission pattern.

ここで重要なことはこの穿孔8bの大きさ(孔
径da)は、放電部の発光効率と輝度に大きく影
響し、該Y電極膨大部8aの外径をdbそした時
に、0.5db≦da≦0.75dbの範囲が最適である。す
なわち、穿孔8bの径daが円形膨大部外径比の
0.5以下では、当該穿孔部と下層のX電極2との
間に小さな放電スポツトしか発生しないので円形
膨大部外周に発生している放電光との間に暗部が
残り、また0.75以上では前述の電極エツジ部にし
か放電が生じないとする放電現象によつて、穿孔
部の中心が発光せずに暗部となり、要するに前記
0.5db≦da≦0.75dbの範囲外においては発光形態
に暗部が生じ、依然として輝度が大きくとれない
わけである。言い換えれば、穿孔径をこの範囲内
に選定すると暗部が全くない形状のシヤープな放
電スポツトを発生することができる。
What is important here is that the size of this perforation 8b (hole diameter da) greatly affects the luminous efficiency and brightness of the discharge part, and when the outer diameter of the Y electrode enlarged part 8a is db, 0.5db≦da≦ A range of 0.75db is optimal. That is, the diameter da of the perforation 8b is the ratio of the outer diameter of the circular ampullae.
If it is less than 0.5, only a small discharge spot will be generated between the perforated part and the lower layer X electrode 2, so a dark area will remain between the discharge light generated around the outer circumference of the circular ampullae, and if it is more than 0.75, the above-mentioned electrode Due to the discharge phenomenon in which discharge occurs only at the edges, the center of the perforation does not emit light and becomes a dark area, in short, as described above.
Outside the range of 0.5 db≦da≦0.75 db, dark portions occur in the light emission form, and it is still not possible to obtain high brightness. In other words, if the perforation diameter is selected within this range, it is possible to generate a sharp discharge spot with no dark areas.

第5図および第6図はこのような発光形態の発
光効率と輝度の実験結果を示した図であり、両図
とも横軸に電極膨大円形部の径をとつている。な
おこの実験は、下層X電極2の円形膨大部外径が
210μm,上層Y電極8の円形膨大部外径が
150μm,両電極の配列ピツチが0.45mm,そして、
ネオン(Ne)とキセノン(Xe)との混合ガスを
圧力500Torrで封入したパネルを用いて行なつ
た。これらの図で明らかなように、上層Y電極8
の円形膨大部8aに90μmの径の孔8bを形成し
た、つまり孔径の円形膨大部外径に対する比率
0.6とした上層電極構造を有するパネルによれば、
穿孔を持たない従来のパネルに比べて発光効率,
輝度ともに約2倍向上した。またこれを最高にし
て発光効率1.2m/w以上,輝度400cd/m2以上
の最適値を呈する77〜110μmの範囲の孔径が有用
であることが確認された。
FIGS. 5 and 6 are diagrams showing the experimental results of the luminous efficiency and luminance of such a light emitting form, and in both figures, the horizontal axis represents the diameter of the large circular electrode portion. Note that in this experiment, the outer diameter of the circular ampullae of the lower X electrode 2 was
210 μm, the outer diameter of the circular ampullae of the upper layer Y electrode 8 is
150μm, the arrangement pitch of both electrodes is 0.45mm, and
The experiment was carried out using a panel filled with a mixed gas of neon (Ne) and xenon (Xe) at a pressure of 500 Torr. As is clear from these figures, the upper layer Y electrode 8
A hole 8b with a diameter of 90 μm was formed in the circular enlarged part 8a, that is, the ratio of the hole diameter to the outer diameter of the circular enlarged part.
According to the panel with the upper layer electrode structure set to 0.6,
Luminous efficiency compared to conventional panels without perforations,
Both brightness has improved by about 2 times. Furthermore, it has been confirmed that a pore diameter in the range of 77 to 110 μm is useful because it maximizes the luminous efficiency and exhibits the optimum values of 1.2 m/w or more and luminance of 400 cd/m 2 or more.

このY電極円形膨大部の孔の径77〜110μmは、
該円形膨大部の外径150μmに対し0.51〜0.73の大
きさであり、その比率は前述の0.5〜0.75にほぼ
対応している。に対し0.5〜0.75の大きさである。
The diameter of the hole in the circular ampullae of this Y electrode is 77 to 110 μm.
The size is 0.51 to 0.73 with respect to the outer diameter of 150 μm of the circular enlarged portion, and the ratio approximately corresponds to the above-mentioned 0.5 to 0.75. The magnitude is between 0.5 and 0.75.

なお、以上の実施例において穿孔8bの形状
は、真円形としたが、本質的には電極円形膨大部
の中心付近が穿孔されておれば角形、あるいは内
縁がギザギザ模様の円形などでも良い。
In the above embodiment, the shape of the perforation 8b is a perfect circle, but it may be rectangular, or circular with a jagged inner edge, etc., as long as the perforation is essentially in the vicinity of the center of the electrode's circular expansion.

(g) 発明の効果 以上の説明から明らかなように、この発明によ
れば、同一基板上に一対の電極を上下に交叉して
対向配置した面放電形式のガス放電パネル構造に
おいて解像度および発光輝度を著しく向上でき、
表示品質の大幅改善を奏することができる。
(g) Effects of the Invention As is clear from the above description, according to the present invention, resolution and luminance can be improved in a surface discharge type gas discharge panel structure in which a pair of electrodes are arranged facing each other on the same substrate, vertically intersecting each other. can be significantly improved,
Display quality can be significantly improved.

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

第1図および第2図は従来の面放電型ガス放電
3ネルの電極配置の一例を示す平面図とそれの
−′線に沿つた断面図、第3図および第4図は
本発明の一実施例に基づくパネルの電極配置を示
す平面図とそれの−′線に沿つた断面図、第
5図および第6図は本発明の効果を説明するため
の上層電極の穿孔径の大小と発光効率および輝度
の関係を示した図である。 図において、1は下側ガラス基板、2は下層電
極、3は誘電体層、4および8は上層電極、5は
絶縁層、6はガス封入空間、7はカバー用上側ガ
ラス基板、2a,4aおよび8aは電極膨大部、
8bは穿孔をそれぞれ示す。
1 and 2 are a plan view showing an example of the electrode arrangement of a conventional surface discharge type gas discharge triple channel, and a cross-sectional view thereof taken along the line -', and FIGS. A plan view showing the electrode arrangement of the panel according to the embodiment, a sectional view thereof taken along the line -', and FIGS. 5 and 6 show the size of the perforation diameter of the upper layer electrode and the light emission for explaining the effects of the present invention. FIG. 3 is a diagram showing the relationship between efficiency and brightness. In the figure, 1 is a lower glass substrate, 2 is a lower electrode, 3 is a dielectric layer, 4 and 8 are upper electrodes, 5 is an insulating layer, 6 is a gas-filled space, 7 is an upper glass substrate for cover, 2a, 4a and 8a is the electrode ampulla;
8b each indicates a perforation.

Claims (1)

【特許請求の範囲】 1 ガス封入空間6を挟んで対向する一対の基板
1,7の一方の基板1上に、絶縁膜3を介して互
いに交差する方向に配列された2層の電極2,8
を有し、その上層電極2を誘電体層により被覆
し、これら上層電極2と下層電極8の交点近傍で
放電を発生させるガス放電パネル構造において、 前記下層電極2および上層電極8の交差部にそ
れぞれ膨大部を形成し、該下層電極2の膨大部2
aは上層電極8の膨大部8aよりも大きな円形を
有し、かつ該上層電極8の膨張部8aは中心が穿
孔されたリング形であつてその孔8bの径を膨大
部外径の0.5〜0.75の比率で形成してなり、当該
上層電極膨大部8aの外周および孔内周において
それぞれ下層電極膨大部2aとの間で放電を発生
させるようにした ことを特徴とする面放電型ガス放電パネル。
[Claims] 1. Two layers of electrodes 2 arranged on one substrate 1 of a pair of substrates 1 and 7 facing each other with a gas-filled space 6 interposed therebetween in a direction crossing each other with an insulating film 3 interposed therebetween. 8
In a gas discharge panel structure in which the upper electrode 2 is covered with a dielectric layer and a discharge is generated near the intersection of the upper electrode 2 and the lower electrode 8, at the intersection of the lower electrode 2 and the upper electrode 8. The enlarged portions 2 of the lower electrode 2 each form an enlarged portion.
a has a circular shape larger than the enlarged part 8a of the upper electrode 8, and the enlarged part 8a of the upper electrode 8 has a ring shape with a hole in the center, and the diameter of the hole 8b is 0.5 to 0.5 to the outer diameter of the enlarged part. A surface discharge type gas discharge panel characterized in that the electrode is formed at a ratio of 0.75, and discharge is generated between the outer circumference of the upper layer electrode enlarged portion 8a and the inner circumference of the hole, respectively, between the upper layer electrode enlarged portion 2a and the lower layer electrode enlarged portion 2a. .
JP59004170A 1984-01-11 1984-01-11 Surface discharge type gas discharge panel Granted JPS60148035A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59004170A JPS60148035A (en) 1984-01-11 1984-01-11 Surface discharge type gas discharge panel

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59004170A JPS60148035A (en) 1984-01-11 1984-01-11 Surface discharge type gas discharge panel

Publications (2)

Publication Number Publication Date
JPS60148035A JPS60148035A (en) 1985-08-05
JPH0346941B2 true JPH0346941B2 (en) 1991-07-17

Family

ID=11577257

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59004170A Granted JPS60148035A (en) 1984-01-11 1984-01-11 Surface discharge type gas discharge panel

Country Status (1)

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JP (1) JPS60148035A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2623405B2 (en) * 1992-04-13 1997-06-25 株式会社ノリタケカンパニーリミテド Color plasma display panel

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS49129476A (en) * 1973-04-11 1974-12-11
JPS49129475A (en) * 1973-04-10 1974-12-11
JPS506276A (en) * 1973-05-17 1975-01-22
JPS5750743A (en) * 1980-09-12 1982-03-25 Okaya Denki Sangyo Kk Gas discharge display panel
JPS5774940A (en) * 1980-10-24 1982-05-11 Fujitsu Ltd Gas discharge panel

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS49129475A (en) * 1973-04-10 1974-12-11
JPS49129476A (en) * 1973-04-11 1974-12-11
JPS506276A (en) * 1973-05-17 1975-01-22
JPS5750743A (en) * 1980-09-12 1982-03-25 Okaya Denki Sangyo Kk Gas discharge display panel
JPS5774940A (en) * 1980-10-24 1982-05-11 Fujitsu Ltd Gas discharge panel

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JPS60148035A (en) 1985-08-05

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