JPS63114022A - Spot knocking method for cathode-ray tube - Google Patents

Spot knocking method for cathode-ray tube

Info

Publication number
JPS63114022A
JPS63114022A JP25898786A JP25898786A JPS63114022A JP S63114022 A JPS63114022 A JP S63114022A JP 25898786 A JP25898786 A JP 25898786A JP 25898786 A JP25898786 A JP 25898786A JP S63114022 A JPS63114022 A JP S63114022A
Authority
JP
Japan
Prior art keywords
grid
anode
ray tube
voltage
cathode
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
JP25898786A
Other languages
Japanese (ja)
Inventor
Wataru Imanishi
今西 渉
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 JP25898786A priority Critical patent/JPS63114022A/en
Publication of JPS63114022A publication Critical patent/JPS63114022A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To remove all portions acting as a field emission source when a cathode-ray tube is operated by repeating the active treatment and spot knocking of a Ba oxide layer stuck to the third grid. CONSTITUTION:First a cathode 15 is heated, a positive voltage is applied to the second grid 13 and the third grid 12 and 0V or negative voltage is applied to an anode 11 respectively, a voltage of 0V-negative several V is applied to the first grid 14, and an electron beam 26 hits the Ba oxide layer 24 on the grid 12 for active treatment. Thereby, the work function on the surface of the layer 24 is reduced, and field emission is mode easy to take place from a minor lug. Next, a high voltage is applied across the grid 12 and the anode 11 to perform spot knocking. Accordingly, discharge occurs between the lug 24 having the small work function and the anode 11, and the lug 24 disappears. By repeating the above process multiple times, all lugs 24 acting as field emission sources can be removed.

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は陰極線管の耐電圧特性を改良するために施す
スポットノッキング方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a spot knocking method applied to improve the withstand voltage characteristics of a cathode ray tube.

し従来の技術] 一般にカラー陰極線管は第3図に示すように、パネル部
(1)、ファンネル部(2)およびネック部(3)から
成るガラスバルブ(4)を有し、このガラスバルブ(4
)の内外面には、内部導電膜(5)および外部導電膜(
6)が設けられている。内部導電膜(5)はネック部(
3)の内面まで延在すると共に、ファンネル部(2)に
は電子銃構体(9)が収納されており、電子銃構体(8
)は第4図に示すように陽極(11)、第3格子(12
)、第2格子(13)、第1格子(14)、カソード(
15)、これらの各電極を一体に保持するビードガラス
(1θ)、カップ状体(17)、およびバルブスペーサ
(18)を具備している。カップ状体(17)のパネル
側にはゲッタ(19)が支持棒(20)により支えられ
ており、このゲッタ(19)は陰極線管の排気工程完了
後、外部から高周波誘導加熱によって加熱され、バリウ
ム粒子(21)を飛散させる。
[Prior Art] Generally, a color cathode ray tube has a glass bulb (4) consisting of a panel part (1), a funnel part (2) and a neck part (3), as shown in FIG. 4
) have an inner conductive film (5) and an outer conductive film (5) on the inner and outer surfaces of the
6) is provided. The internal conductive film (5) has a neck part (
3), and an electron gun assembly (9) is housed in the funnel part (2).
) has an anode (11) and a third grating (12) as shown in Figure 4.
), second grating (13), first grating (14), cathode (
15), a bead glass (1θ) for holding these electrodes together, a cup-shaped body (17), and a bulb spacer (18). A getter (19) is supported by a support rod (20) on the panel side of the cup-shaped body (17), and after the evacuation process of the cathode ray tube is completed, this getter (19) is heated from the outside by high-frequency induction heating. The barium particles (21) are scattered.

このバリウム粒子飛散時の管内の真空度は10−3To
rr以上にも達するので、ゲッタ(18)の前面にバリ
ウム粒子の雲(22)ができ、ここで反射されたバリウ
ム粒子(21)の一部分が第5図に示すように陽極(1
1)の電子ビーム孔を通過し、第3格子(12)の陽極
(11)側の電子ビーム通過孔の周面に蒸着してバリウ
ム層を形成する。そうして、その後の陰極線管の製造工
程で酸素ガスによって酸化さ  ごれ酸化バリウムの層
(24)となる。
The degree of vacuum inside the tube during barium particle scattering is 10-3To
rr or more, a cloud of barium particles (22) is formed in front of the getter (18), and a part of the barium particles (21) reflected from this cloud reaches the anode (1) as shown in FIG.
The barium layer passes through the electron beam hole of 1) and is deposited on the circumferential surface of the electron beam passage hole on the anode (11) side of the third grating (12). Then, in the subsequent manufacturing process of the cathode ray tube, it is oxidized by oxygen gas and becomes a barium oxide layer (24).

この酸化バリウム層(24)は陰極線管の動作時におい
て、フィールドエミッションの発生源となることがある
。すなわち、動作中は陽極(11)tこ25〜27KV
、第3格子(12)ニ4 、5〜9 KV程度の電圧が
印加されているので、第3格子(12)と陽極(11)
との間には18〜21KV程度の電圧が印加されること
になる。第3格子(12)には、微少な突起物(25)
が存在することは避けられず、この突起1(25)の周
囲から第3格子(12)と陽極(11)間に印加された
18〜20KVの電圧によってフィールドエミッション
が発生すると、陰極線管の蛍光面の不必要な部分を発光
させ、映像の品位を低下させる。このフィールドエミッ
ションの密度は一般に次のようなFowl er −N
ordheimの関係式によって示される。
This barium oxide layer (24) may become a source of field emissions during operation of the cathode ray tube. That is, during operation, the anode (11) has a voltage of 25 to 27 KV.
, the third grid (12) 4, Since a voltage of about 5 to 9 KV is applied, the third grid (12) and the anode (11)
A voltage of about 18 to 21 KV will be applied between the two. The third lattice (12) has minute protrusions (25).
It is unavoidable that there is a This causes unnecessary parts of the screen to emit light, reducing the quality of the image. The density of this field emission is generally calculated as Fowl er −N
It is shown by the ordheim relational expression.

ここで、Jはフィールドエミッション密度、βは突起部
の電界倍増係数、Eは第3格子(12)と陽極(11)
の電界、φは第3格子面の仕事函数である。
Here, J is the field emission density, β is the electric field multiplication coefficient of the protrusion, and E is the third grating (12) and the anode (11).
electric field, φ is the work function of the third lattice plane.

この式からフィールドエミッションJはβ、Eが大きく
なる程、φが小さくなる程大きくなることがわかる。
From this equation, it can be seen that the field emission J becomes larger as β and E become larger, and as φ becomes smaller.

[発明が解決しようとする問題点] 第6図は第5図の第3格子(12)と陽極(11)付近
の拡大断面図で、第3格子(12)の一部に突起物(2
5)があり、その上にゲッタ(18)からの酸化ノくリ
ウム層(24)が付着している。このような状態で第3
格子(12)と陽極(11)間に20KV程度の高電圧
が印加されると、突起物(25)の先端は電界倍増係数
βが大きく、仕事函数φが小さいので上式に示すように
フィールドエミッションが発生する。これを取除くため
陰極線管の製造工程中に、動作時に印加される高電圧の
2〜3倍程度の高電圧を印加して強制的に放電させるス
ポットノッキングを行っている。この処理によって大き
な突起物(25)は順次取除かれていくが、小さなもの
は残っている。このような状態の陰極線管を作動させる
と、散乱した電子ビームの一部が酸化バリウム層(24
)の表面を衝撃して酸化バリウムを活性化する。酸化バ
リウム層(24)の仕事函数φは1.7eV程度である
が、電子ビームの衝撃により活性化されると仕事函数φ
は1.2eV程度に低下するので、それまでフィールド
エミッションが↑ていないところから新たにフィールド
エミッションが放出され、映像の品質が低下するという
問題点があった。
[Problems to be Solved by the Invention] FIG. 6 is an enlarged sectional view of the vicinity of the third lattice (12) and anode (11) in FIG.
5), on which is deposited a layer of notrium oxide (24) from the getter (18). In this situation, the third
When a high voltage of about 20 KV is applied between the grating (12) and the anode (11), the tip of the protrusion (25) has a large electric field multiplication factor β and a small work function φ, so the field changes as shown in the above equation. Emissions occur. In order to eliminate this, spot knocking is performed during the manufacturing process of cathode ray tubes, in which a high voltage approximately two to three times higher than that applied during operation is applied to force a discharge. Through this process, large protrusions (25) are successively removed, but small ones remain. When a cathode ray tube is operated in such a state, some of the scattered electron beams are absorbed into the barium oxide layer (24
) to activate barium oxide. The work function φ of the barium oxide layer (24) is approximately 1.7 eV, but when activated by electron beam impact, the work function φ increases.
Since this decreases to about 1.2 eV, new field emissions are emitted from areas where there was no field emission up to that point, causing a problem in that the quality of the image deteriorates.

この発明は上記ような問題点を解消するためになされた
もので、陰極線管の作動中において新たなフィールドエ
ミッションが生じることのないスポットノッキング方法
を得ることを目的とする。
The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to provide a spot knocking method that does not generate new field emissions during operation of a cathode ray tube.

[問題点を解決するための手段] この発明に係るスポットノッキング方法は、まず陽極に
Ovまたは負の電圧を印加し、第3格子に200〜60
0Vの電圧を印加して第3椙子電流を流し、当該第3格
子に付着している酸化バリウム層を活性化する活性化処
理と、第3格子および第3格子の陽極側端部に電子衝撃
し、酸化バリウム表面を活性化陽極に高電圧を印加する
スポットノッキング処理とを交互に複数回施すようにし
たスポットノッキング方法である。
[Means for solving the problem] In the spot knocking method according to the present invention, first, Ov or a negative voltage is applied to the anode, and a voltage of 200 to 60 V is applied to the third grid.
An activation process is performed in which a voltage of 0V is applied to cause a third current to flow, activating the barium oxide layer attached to the third lattice, and electrons are applied to the third lattice and the anode side end of the third lattice. This is a spot-knocking method in which a spot-knocking treatment in which a high voltage is applied to an anode that activates the barium oxide surface is alternately performed multiple times.

[作用] この発明における活性化処理によって第3格子に付着し
ている酸化バリウム層が活性化され、ついて施される。
[Function] The barium oxide layer adhering to the third lattice is activated by the activation treatment in the present invention, and the barium oxide layer is then applied.

スポットノッキングによってフィールドエミッションを
発生するようになった部分が除去され、この活性化処理
とスポットノッキングを繰返すことにより、陰極線管を
作動させたときにフィールドエミッション源となる部分
をすべて取除くことができる。
Spot knocking removes the parts that generate field emissions, and by repeating this activation process and spot knocking, it is possible to remove all parts that become field emission sources when the cathode ray tube is operated. .

[発明の実施例] 以下、この発明の実施例を第1図および第2図によって
説明する。第1図は電子銃構体(9)の縦断面図、第2
図はその第3格子と陽極部分の拡大断面図である。
[Embodiments of the Invention] Examples of the invention will be described below with reference to FIGS. 1 and 2. Figure 1 is a longitudinal sectional view of the electron gun assembly (9), Figure 2
The figure is an enlarged sectional view of the third lattice and anode portion.

まず、カソード(15)を加熱し、第2格子(13)お
よび第3格子(12)には200〜600Vの電圧を、
陽極(11)にはOvまたは負の電圧をそれぞれ印加し
、第1格子(14)にはOV〜負の数Vの電圧を印加し
て第3格子が赤熱されない程度の第3格子電流を通して
電子ビーf、(2B)を第3格子(12)の酸化バリウ
ム層(24)に衝突させる活性化処理を施す。これによ
り、酸化バリウム層(24)の表面の仕事函数φを1.
7eV程度から1.2eV程度まで低下させて微小な突
起からフィールドエミッションを放出しやすい状態とす
る。つぎに60〜70KVの高電圧を第3格子(12)
と陽極(11)間に印加するスポットノッキングを施す
。これにより。
First, the cathode (15) is heated, and a voltage of 200 to 600V is applied to the second grid (13) and third grid (12).
A voltage of Ov or a negative voltage is applied to the anode (11), a voltage of OV to a negative number V is applied to the first grid (14), and electrons are passed through the third grid current to an extent that the third grid does not become red hot. An activation process is performed in which the beam f, (2B) collides with the barium oxide layer (24) of the third lattice (12). This reduces the work function φ of the surface of the barium oxide layer (24) to 1.
The voltage is lowered from about 7 eV to about 1.2 eV to create a state in which field emission is easily emitted from minute protrusions. Next, apply a high voltage of 60 to 70 KV to the third grid (12).
Spot knocking is applied between the anode (11) and the anode (11). Due to this.

仕事函数φが小さくなっている突起物(24)と陽極(
11)との間で放電が発生してその突起部(24)が消
滅し、将来陰極線管の動作中に発生するであろうフィー
ルドエミッション源を取除くことができる。
The protrusion (24) with a small work function φ and the anode (
11), the protrusion (24) disappears, and a source of field emissions that may occur in the future during operation of the cathode ray tube can be removed.

しかし、スポットノッキング処理中には多くの放電が発
生し、これにより多情の酸素等のガスが放出され、前に
施した活性化処理によって活性化されていた酸化バリウ
ム層(24)の表面は酸素ガスなどの為、元の状態に戻
ってしまい、以後放電させることができなくなる。そこ
で再び前述した活性化処理を施し、ついでスポットノッ
キング処理を施すという操作を4〜5回繰返すことによ
りフィールドエミッション源となる突起部(24)をす
べて除去することができ、より高品位の陰極m管を得る
ことができる。
However, during the spot knocking process, many discharges occur, which releases a large amount of gas such as oxygen, and the surface of the barium oxide layer (24), which had been activated by the previous activation process, is exposed to oxygen. Due to gas, etc., it will return to its original state and will no longer be able to be discharged. Therefore, by repeating the above-mentioned activation treatment and then spot knocking treatment 4 to 5 times, all the protrusions (24) that become field emission sources can be removed, resulting in a higher quality cathode m You can get the tube.

尚、上記実施例では、ネック部に取付けたネックゲッタ
を有する陰極線管を例に説明したが、ファンネルゲッタ
を有する陰極線管にも同月に適用でき、同様の効果が得
られることはいうまでもない。
In the above embodiment, a cathode ray tube having a neck getter attached to the neck portion was explained as an example, but it goes without saying that the present invention can also be applied to a cathode ray tube having a funnel getter, and similar effects can be obtained.

[発明の効果] 以上のように、この発明は第3格子電流を流して第3格
子に付着した酸化バリウム層を活性化する活性化処理と
、この活性化処理ののち考該第3格子と陽極との間に高
電圧を印加するスポットノッキング処理とを複数回繰返
して施すようにしたスポットノッキング方法であるから
陰極線管の動作中にフィールドエミッションが増加して
陰極線管の品位を低下させることがなく良好な耐電圧特
性を持った陰極線管を得ることができる。
[Effects of the Invention] As described above, the present invention includes an activation process in which a third lattice current is applied to activate the barium oxide layer attached to the third lattice, and after this activation process, the third lattice is Since the spot knocking method involves repeating the spot knocking process by applying a high voltage between the cathode and the anode, field emissions increase during the operation of the cathode ray tube and reduce the quality of the cathode ray tube. Therefore, it is possible to obtain a cathode ray tube with good withstand voltage characteristics.

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

第1図はこの発明の一実施例を説明するための電子銃の
縦断面図、第2図はその第3格子と陽極部分の一部拡大
図、第3図は陰極線管の一部破断側面図、第4図はその
電子銃部分の拡大図、第5図は従来のスポットノッキン
グ方法を説明するための電子銃の縦断面図、第6図はそ
の第3格子と陽極部分一部拡大図である。 (8)・・・電子銃、(11)・・・陽極、(12)・
・・第3格子、(15)・・・カンード、(19)・・
・ゲッタ、(24)・・・酪化/ヘリウム層、(25)
・・・突起部。 なお、各図中、同一符号は同一または相当部分を示して
いる。
Fig. 1 is a longitudinal sectional view of an electron gun for explaining one embodiment of the present invention, Fig. 2 is a partially enlarged view of the third grid and anode portion thereof, and Fig. 3 is a partially broken side view of the cathode ray tube. Figure 4 is an enlarged view of the electron gun part, Figure 5 is a vertical cross-sectional view of the electron gun to explain the conventional spot knocking method, and Figure 6 is a partially enlarged view of the third grid and anode part. It is. (8)...electron gun, (11)...anode, (12)...
...Third lattice, (15)...Cand, (19)...
・Getter, (24)...butyrication/helium layer, (25)
···protrusion. In each figure, the same reference numerals indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] (1)陰極線管の第3格子とカソード間に電圧を印加し
て第3格子電流を流す活性化工程と、この活性化工程を
施したのち上記第3格子と陽極との間に高電圧を印加す
るスポットノッキング工程とを複数回繰返して施すよう
にした陰極線管のスポットノッキング方法。
(1) An activation process in which a voltage is applied between the third grid and the cathode of the cathode ray tube to flow a third grid current; and after this activation process, a high voltage is applied between the third grid and the anode. A spot knocking method for a cathode ray tube in which a spot knocking step of applying an electric current is repeated multiple times.
JP25898786A 1986-10-30 1986-10-30 Spot knocking method for cathode-ray tube Pending JPS63114022A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25898786A JPS63114022A (en) 1986-10-30 1986-10-30 Spot knocking method for cathode-ray tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25898786A JPS63114022A (en) 1986-10-30 1986-10-30 Spot knocking method for cathode-ray tube

Publications (1)

Publication Number Publication Date
JPS63114022A true JPS63114022A (en) 1988-05-18

Family

ID=17327778

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25898786A Pending JPS63114022A (en) 1986-10-30 1986-10-30 Spot knocking method for cathode-ray tube

Country Status (1)

Country Link
JP (1) JPS63114022A (en)

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