JPS62150640A - Flat matrix type cathode-ray tube - Google Patents

Flat matrix type cathode-ray tube

Info

Publication number
JPS62150640A
JPS62150640A JP29102885A JP29102885A JPS62150640A JP S62150640 A JPS62150640 A JP S62150640A JP 29102885 A JP29102885 A JP 29102885A JP 29102885 A JP29102885 A JP 29102885A JP S62150640 A JPS62150640 A JP S62150640A
Authority
JP
Japan
Prior art keywords
glass
spacer
face
coated
bottom plate
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.)
Pending
Application number
JP29102885A
Other languages
Japanese (ja)
Inventor
Nobuo Terasaki
寺崎 信夫
Shuji Iwata
修司 岩田
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP29102885A priority Critical patent/JPS62150640A/en
Publication of JPS62150640A publication Critical patent/JPS62150640A/en
Pending legal-status Critical Current

Links

Landscapes

  • Vessels, Lead-In Wires, Accessory Apparatuses For Cathode-Ray Tubes (AREA)
  • Cathode-Ray Tubes And Fluorescent Screens For Display (AREA)

Abstract

PURPOSE:To prevent the unnecessary discharge along the surface of a spacer glass, and to supplement the function as an acceleration electrode and unify the diffusion of electron beams so as to improve the luminous level, by coating an electroconductive layer of carbon or the like at the upper portion at a face glass side of the spacer glass facing to the bottom plate glass side. CONSTITUTION:At the upper portion of a spacer glass 3 at a face glass side, an electroconductive layer 4 of carbon or the like is coated facing to a bottom plate glass 2 side. The electroconductive layer 4 is coated up to about the middle portion between the face glass 1 and the bottom plate glass 2. Therefore, a specific resistance is given by the coating of the conductive layer 4 to prevent the unnecessary discharge along the surface of the spacer glass 3 and to maintain a specific potential, so that the function of screening plates 1b as acceleration electrodes is supplemented and the diffusion property of electron beams can be exercised. Therefore, the diffusion of the electron beams is made even and the decrease of the luminous level at the periphery of the face glass 1 can be prevented.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、大型画像光示装置のライティングエレメン
トとして用いられるフラットマトリクスCRTに関し、
特に表示面周辺部の発光レベルの向上を図るものである
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a flat matrix CRT used as a lighting element of a large image display device.
In particular, the aim is to improve the level of light emitted at the periphery of the display surface.

〔従来の技術〕[Conventional technology]

第2図は既に提案されているフラットマトリクスCRT
の主要部の構成を示す断面図で、(1)は内側に螢光体
をそれぞれ塗布してなる複数個のアノード電極(1a)
及び電極間をしやへいするしやへい板(1b)を取付け
たフェースガラス、(2)はフィラメント(2a)、お
よびこのフィラメントから放出される電子ビームを上記
アノード電極(1a)に向けて加速するX電極(2b)
とX電極(2C)とでなるグリッド電極を取付けた底板
ガラス、(8)は螢光体を覆うようにしてフェースガラ
ス(1)と底板ガラス(2)とに融着されて一体形成さ
れ上記底板ガラス(2)に向けて窄まった箱状のガラス
容器を形成するスペーサガラスである。
Figure 2 shows a flat matrix CRT that has already been proposed.
(1) is a cross-sectional view showing the configuration of the main parts of the anode electrode (1a), which is formed by coating the inside with a phosphor.
(2) is a filament (2a), and the electron beam emitted from this filament is accelerated toward the anode electrode (1a). X electrode (2b)
The bottom plate glass (8) is integrally formed by being fused to the face glass (1) and the bottom plate glass (2) so as to cover the phosphor. This is a spacer glass that forms a box-shaped glass container that narrows toward the bottom glass (2).

上記の如く構成のフラットマトリクスCRTにおいて、
X電極(2b)とX電極(2C)は走査電極と画素電極
を形成し、4×47) IJクス構造でなり、これに対
応するアノード電極(1a)の塗布された螢光体はそれ
ぞれ所定の位置で赤、緑、青色用のいずれかの螢光体が
塗布されていて、1つのエレメント内の16画素に赤、
緑、青を色付けされている0 しかして、これらの画素を任意に選択するには、各走査
電極と画素電極に各々電圧を印加すれば良く、両電極に
電圧が印加されている部分のみが発光するようになされ
ている。これは、周知の如く、フィラメントより放出さ
れる電子が走査電極と画素電極のグリッド電極に印加さ
れる電圧によって加速され、高圧を印加したアノードに
目がけて衝突することにより、アノード電極面に例えば
塗布された螢光体がこの時の衝突エネルギーにより発光
するものである。
In the flat matrix CRT configured as above,
The X electrode (2b) and the X electrode (2C) form a scanning electrode and a pixel electrode, and have a 4 x 47) IJ structure, and the phosphor coated on the corresponding anode electrode (1a) has a predetermined shape. A phosphor for red, green, or blue is coated at the position of 16 pixels in one element.
Colored green and blue 0 However, in order to arbitrarily select these pixels, it is sufficient to apply a voltage to each scanning electrode and pixel electrode, and only the part where voltage is applied to both electrodes is selected. It is made to emit light. As is well known, the electrons emitted from the filament are accelerated by the voltage applied to the scanning electrode and the grid electrode of the pixel electrode, and collide with the anode to which a high voltage is applied, causing the electrons to strike the anode electrode surface, for example. The coated phosphor emits light due to the collision energy at this time.

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

しかるに、上述した如くフラットマトリクスCRTにお
いては、スペーサガラス(8)の周辺部じゃへい板(1
b)の長さを長くすると、グリッド電極間との距離が短
かくなるためガラス表面に沿って放電するという現象が
生じ、逆に電極間距離を短かくすると、スペーサガラス
(8)上部側面に電荷が帯電し易く加速電極としての機
能が弱まって電子ビームの拡散が弱まるためにフェース
ガラス(1)の最外側周辺部での発光レベルの低下をま
ねいていた0 そこで、この発明は上記の如く問題点を解消するために
なされたもので、スペーサガラス表面に沿う放電現象が
発生することなく、かつフェースガラス最外部周辺部で
の発光レベルをも向上することができるフラットマトリ
クスCRTf提供するものである。
However, as mentioned above, in the flat matrix CRT, the peripheral part of the spacer glass (8) is
If the length of b) is increased, the distance between the grid electrodes will be shortened, causing a phenomenon of discharge along the glass surface. Conversely, if the distance between the electrodes is shortened, the distance between the grid electrodes will be shortened, causing discharge to occur along the top side of the spacer glass (8). The present invention has been developed as described above because it is easily charged and its function as an accelerating electrode is weakened, which weakens the diffusion of the electron beam. This was done to solve the problem, and it provides a flat matrix CRTf that can improve the light emission level around the outermost part of the face glass without causing a discharge phenomenon along the surface of the spacer glass. be.

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

この発明に係るフラットマトリクスCRTは、スペーサ
ガラスのフェースガラス側上部に底板ガラス側に向けて
カーボン等の導電層を塗布したものである。
The flat matrix CRT according to the present invention has a conductive layer of carbon or the like coated on the upper part of the spacer glass on the face glass side toward the bottom glass side.

〔作用〕[Effect]

この発明のフラットマトリクスCRTによれば、スペー
サガラスへのカーボン等の導電層の塗布によυ所定の抵
抗値を付与してスペーサガラス沿面での放電を防止する
ことができると共に、所定の電位を保って電子ビームの
拡散機能を営むことができ、したがってフェースガラス
周辺部での発光レベルの低下を防止できる。
According to the flat matrix CRT of the present invention, by applying a conductive layer such as carbon to the spacer glass, a predetermined resistance value can be imparted to prevent discharge along the surface of the spacer glass, and a predetermined potential can be applied to the spacer glass. It is possible to perform the function of diffusing the electron beam while maintaining the electron beam, thereby preventing a decrease in the light emission level around the face glass.

〔実施例〕〔Example〕

以下、この発明の一実施例を第2図と同一部分は同一符
号を付して示す第1図に基いて説明する。
Hereinafter, one embodiment of the present invention will be described with reference to FIG. 1, in which the same parts as in FIG. 2 are denoted by the same reference numerals.

この第1図において、第2図と異なる点は、スペーサガ
ラス(8)の7エースガラス(1)側止部に底板ガラス
(2)側に向けてカーボン等の導電層(4)を塗布した
点で、その他は同様である。なお、上記導電層(4)は
フェースガラス(1)と底板ガラス(2)間の略中間位
置まで塗布しである。
The difference between Fig. 1 and Fig. 2 is that a conductive layer (4) of carbon or the like is applied to the stop on the 7 ace glass (1) side of the spacer glass (8) toward the bottom glass (2). In other respects, they are the same. Note that the conductive layer (4) is applied to approximately the middle position between the face glass (1) and the bottom glass (2).

したがって、上記実施例によれば、導電層(4)の塗布
によって所定の抵抗値を付与してスペーサガラス(8)
の沿面での不要放電を防止し、かつ所定の電位を保持さ
せることができじゃへい板(1b)の加速電極としての
働きを補い電子ビームの拡散機能を営むことができるた
め、拡散が均一になりフェースガラス(1)周辺部での
発光レベルの低下を防止できる。
Therefore, according to the above embodiment, a predetermined resistance value is imparted to the spacer glass (8) by coating the conductive layer (4).
It is possible to prevent unnecessary discharge along the creeping surface of the electron beam and to maintain a predetermined potential, which complements the function of the baffle plate (1b) as an accelerating electrode and performs the function of diffusing the electron beam, resulting in uniform diffusion. Therefore, it is possible to prevent a decrease in the light emission level in the periphery of the face glass (1).

〔発明の効果〕〔Effect of the invention〕

以上のようにこの発明によれば、スペーサガラスのフェ
ースガラス側上部に底板ガラス側に向けてカーボン等の
導電層を塗布したことによシ、スペーサガラス沿面での
不要放電を防止し、かつ加速電極としての働きを補い電
子ビームの拡散を均一にして発光レベルの向上を図るこ
とができる。
As described above, according to the present invention, by applying a conductive layer such as carbon to the upper part of the face glass side of the spacer glass toward the bottom glass side, unnecessary discharge along the surface of the spacer glass can be prevented and accelerated. It can supplement the function of an electrode and uniformly diffuse the electron beam, thereby improving the light emission level.

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

第1図はこの発明の一実施例を示す概略断面図、第2図
はこの発明の前提技術としての概略断面図でる秦。 図中、(1)はフェースガラス、(1a)はアノード電
極、(1b)はじやへい板、(2)は底板ガラス、(2
a)はフィラメント、(2b)U X 1M、極(グリ
ッド)、(2C)ij、Y電極(グリッド)、(8)は
スペーサガラス、(4)は導電層である。 なお、図中、同一符号は同−又は相当部分を示す0
FIG. 1 is a schematic sectional view showing an embodiment of the present invention, and FIG. 2 is a schematic sectional view showing a basic technology of the present invention. In the figure, (1) is the face glass, (1a) is the anode electrode, (1b) is the front plate, (2) is the bottom plate glass, (2)
a) is a filament, (2b) is a U x 1M pole (grid), (2C) is a Y electrode (grid), (8) is a spacer glass, and (4) is a conductive layer. In addition, in the figures, the same symbols indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 内側に螢光体をそれぞれ塗布してなる複数個のアノード
電極及びアノード電極間をしゃへいするしゃへい板を取
付けたフェースガラスと、フィラメントおよびこのフィ
ラメントから放出される電子ビームを上記アノード電極
に向けて加速するグリッド電極を取付けた底板ガラスと
、上記螢光体を覆うようにして上記フェースガラスと底
板ガラスとに一体に形成されて該底板ガラスに向けて窄
まった箱状のガラス容器を形成するスペーサガラスとを
備えると共に、このスペーサガラスのフェースガラス側
上部に底板ガラス側に向けてカーボン等の導電層を塗布
したことを特徴とするフラットマトリクスCRT。
A face glass equipped with a plurality of anode electrodes each coated with a fluorescent material on the inside, a shielding plate for shielding between the anode electrodes, a filament, and an electron beam emitted from the filament is accelerated towards the anode electrode. a spacer that is integrally formed with the face glass and the bottom glass so as to cover the phosphor and forms a box-shaped glass container that narrows toward the bottom glass; A flat matrix CRT characterized in that a conductive layer of carbon or the like is coated on the upper part of the spacer glass on the face glass side toward the bottom glass side.
JP29102885A 1985-12-24 1985-12-24 Flat matrix type cathode-ray tube Pending JPS62150640A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29102885A JPS62150640A (en) 1985-12-24 1985-12-24 Flat matrix type cathode-ray tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29102885A JPS62150640A (en) 1985-12-24 1985-12-24 Flat matrix type cathode-ray tube

Publications (1)

Publication Number Publication Date
JPS62150640A true JPS62150640A (en) 1987-07-04

Family

ID=17763512

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29102885A Pending JPS62150640A (en) 1985-12-24 1985-12-24 Flat matrix type cathode-ray tube

Country Status (1)

Country Link
JP (1) JPS62150640A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01320743A (en) * 1988-06-22 1989-12-26 Matsushita Electric Ind Co Ltd Image display device
EP0365686A1 (en) * 1988-03-29 1990-05-02 Sony Corporation Fluorescent display tube
JPH0391652U (en) * 1989-12-28 1991-09-18
US6377002B1 (en) 1994-09-15 2002-04-23 Pixtech, Inc. Cold cathode field emitter flat screen display

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5315751A (en) * 1976-07-28 1978-02-14 Ise Electronics Corp Fluorescent display tube

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5315751A (en) * 1976-07-28 1978-02-14 Ise Electronics Corp Fluorescent display tube

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0365686A1 (en) * 1988-03-29 1990-05-02 Sony Corporation Fluorescent display tube
JPH01320743A (en) * 1988-06-22 1989-12-26 Matsushita Electric Ind Co Ltd Image display device
JPH0391652U (en) * 1989-12-28 1991-09-18
US6377002B1 (en) 1994-09-15 2002-04-23 Pixtech, Inc. Cold cathode field emitter flat screen display

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