JPS6243302B2 - - Google Patents
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- Publication number
- JPS6243302B2 JPS6243302B2 JP5200778A JP5200778A JPS6243302B2 JP S6243302 B2 JPS6243302 B2 JP S6243302B2 JP 5200778 A JP5200778 A JP 5200778A JP 5200778 A JP5200778 A JP 5200778A JP S6243302 B2 JPS6243302 B2 JP S6243302B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- grid
- electron gun
- electron
- voltage
- 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
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- 239000003990 capacitor Substances 0.000 claims description 4
- 230000002093 peripheral effect Effects 0.000 claims description 3
- 238000010894 electron beam technology Methods 0.000 description 20
- 230000005686 electrostatic field Effects 0.000 description 4
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 125000006850 spacer group Chemical group 0.000 description 2
- 230000004075 alteration Effects 0.000 description 1
- 239000003086 colorant Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
Description
【発明の詳細な説明】
本発明は複数本の電子ビームを射出する電子銃
に係り、特に前記電子ビームをターゲツト上に極
めて精度よく集束することが可能な電子銃の構造
に関するものである。
例えば複数本の電子ビームを射出する電子銃を
内装する通常のカラー受像管に於ては、前記各電
子ビームがそれぞれの電子レンズを通つて、前記
カラー受像管のフエースプレート内面に被着形成
されたドツト状または帯状の赤、緑、青各色を発
光する螢光体層からなるターゲツトの所定の螢光
体層にそれぞれ集束されるようになされている。
この場合前記電子レンズは一般に静電界により形
成されており、電子ビームが前記静電界を通過す
る間に集束されることになる。前記静電界は電子
ビームの径路に直角に配置され、かつ電子ビーム
の通る開孔部を有する少なくとも2個の対設する
電極間に形成され、この静電界により作られた電
子レンズの特性は普通前記対設する電極間に印加
される電圧と距離及び電子ビームの通る開孔部の
寸法などにより変えることができる。
また電子銃の性能は前記電子レンズの倍率及び
球面収差が小さい程良いとされており、このため
長焦点距離を有する電子レンズとすることが必要
となるが、最も効果的な電極間電圧による方法は
一般にはカラー受像管のベースに植設されたステ
ムピン部で互いに放電を起さない範囲としなくて
はならないし、また電子ビームの通る開孔部の寸
法も、カラー受像管のネツク部内径が他の電気的
条件から制約を受けるため、任意に大きく設計す
ることは出来ないし、更に対設する電極間の距離
を大きくすることは、前記ネツク部の内壁に生じ
る浮遊電界や電子銃内の他の不所望な電界によつ
て電子レンズの特性が影響を受けるので、これも
適当ではない。いずれにしても電子レンズの設計
はカラー受像管の設計によつて定められる物理的
条件によつて制約を受ける。このことは特にカラ
ー受像管の場合、多電子ビームを必要とするので
前記制約は特に著しくなる。
前述したような種々の制約を回避するための一
般的な傾向は、長焦点距離電子レンズを作るため
に、電極電圧および電極数を許容される範囲内で
組合わせることである。例えば特開昭51−76072
号公報、特開昭51−77061号公報に述べられてい
る電子銃などがこの例である。
これらの例にみられるように電極電圧、電極の
種類を組合わせる方法は一般に電子銃の構造を複
雑にしたり、電子レンズを形成させるために、更
の他の電圧を附与しなければならず、経済性を損
うのが常である。
また一般に電子レンズの性能を向上させるため
には、附与すべき電圧は前記例も含めて高くしな
ければならず、それに伴つて、カラー受像管のベ
ース部分での放電を防止し、このカラー受像管を
内装したテレビジヨン受像機の信頼性を確保する
ために特別の工夫を施す必要があり、更に経済性
を低下させることになる。
前述した欠点を解消する為に発明者は先に電子
レンズは高電圧集束設計ではあるが、カラー受像
管に外部から附与する電圧はそれより低い電子銃
を出願した。次に第1図a,b、第2図及び第3
図によりその構造及び等価回路を説明する。
図に示す電子銃の基本形式はよく知られたユニ
ポンテンシヤル形インライン電子銃であり、電子
銃1は複数個の電極と、それらを支持する複数の
ガラス支持棒10からなり、前記複数個の電極は
3個の陰極2,3,4、第1グリツド5、第2グ
リツド6、第1集束グリツド即ち第3グリツド7
第2集束グリツド即ち第4グリツド8、第2集束
グリツド即ち第5グリツド9の順に前記ガラス棒
10に取付けられている。前記3個の陰極2,
3,4は同一平面上の3本のビームの径路に沿つ
て電子ビームを射出し、前記第1グリツド5と第
2グリツド6は近接配置された平板状電極で、そ
れぞれ各電子ビーム径路と整合した3個の開孔部
を有し、第3グリツド2は第2グリツド6に近接
配置され、開放端で接合された2個のカツプ2
0,21よりなり、このカツプ21,21の閉塞
端には、それぞれ各電子ビーム径路に整合した3
個の電子ビーム開孔部が設けられている。
前記第1のカツプ20の開孔部17,18,1
9は第2グリツド6の開孔部より径大であり、第
2のカツプ21の開孔部22,23,24は第1
のカツプ20の開孔部より更に大きくなつてい
る。
また第4グリツド8は少なくとも3個の補助電
極よりなり、第1の電極25と第2の電極27は
それぞれ2個のカツプ状電極を接合して成り、そ
れぞれ各電子ビーム径路に整合した3個の開孔部
が設けられている。この第1の電極25と、第2
の電極27は電気的に接続され同電位である。
前記第1の電極25と第2の電極27は互に電
子ビームの径路方向に離間しており、かつその間
隙の中間部に第3の板状電極26(以下単に第3
の電極と称す)が配置され、この第3の電極26
にも各電子ビーム径路に整合した3個の開孔部が
設けられている。第5グリツド9は第3グリツド
7と第4グリツド8間の距離とほぼ等しい距離だ
け第4グリツド8より離間して配置されており、
少なくとも3個の各電子ビーム径路に整合した3
個の開孔部が設けられたカツプ状電極より成つて
いる。この第5グリツド9の3個の開孔部36,
37,38のうち中央の開孔部37は第1グリツ
ド5から第4グリツド8までの開孔部と整合して
いるが、両側の開孔部36,38は夫々中央開孔
部37から外方に離れるように僅かに偏位してい
る。第5グリツド9には更に各電子ビーム径路に
略整合した3個の開孔部をその底部に有する有底
筒状のコンバージエスカツプ42が取付けられて
いる。このコンバージエンカツプ42の開口側端
部には外方向に突出した3個の金属条よりなるバ
ルブスペーサ45が取付けられている。
この様な構造を有する電子銃に於て、第3グリ
ツド7と第5グリツド9を接続し、バルブスペー
サ45を介して陽極電圧を印加し、第4グリツド
8の第1の電極25と第2の電極27を接続し、
特に電圧を印加せず、第3の電極26を例えば接
地した時を考えて見ると、前記第1の電極25、
第2の電極27には前記第3グリツド7と第1の
電極25との対設面間の間隔G1と前記第1の電
極25と前記第3の電極26との対設面間の間隔
G2とによりほぼ決定されるコンデンサC1及びC2
によつて発生する電位が集束電圧として印加され
ることになる。この場合第3の電極26はなるべ
くならば電子銃の集束電圧に大きく影響を与えな
いように設計されている。
即ち第3の電極26には例えば零ボルトの電圧
を与え、陽極即ち第3グリツド7及び第5グリツ
ド9にはE=25KV、第4グリツド8の第1の電
極25第2の電極27の電圧e2が9KVであれば、
第3図の等価回路からも明らかなようにG1/G2
=1/0.6程度に選択すればよいことになるが、
ここでG1/G2の間隔比はそれぞれの電極の対設
部形状によつて変化するため、一概にG1/G2=
1/0.6とはならない。
即ち前述した構造を有する電子銃に於ては、外
部から附与する電圧が低いにもかかわらず、前述
した所望の電子銃としての性能は具備している点
では優れているが、集束電極即ち第1の電極25
及び第2の電極27の電位が不安定であること、
即ちカラー受像管の動作スタート時と長時間動作
後の第1の電極25と第2の電極27に与えるべ
き電圧が変化しやすいと云う欠点があつた。
本発明は前記欠点に鑑みなされたものであり、
先願の不具合を除去し、カラー受像管の動作スタ
ート時から長時間動作後迄一定な集束電圧を得る
ことが出来る電子銃の構造に関するものである。
次に第4図によつて本発明の一実施例を説明す
る。図中前記先願と同一符号は同一部分を示し特
に説明を加えない。
即ち第1集束グリツドすなわち第3グリツド7
と、第3集束グリツド即ち第5グリツド9は接続
され陽極電圧が印加されており、第4グリツド8
の第1の電極25と第2の電極27は互いに接続
され、特に電圧は印加してなく、前記第1の電極
25と第2の電極27の間に間挿された第3の電
極26には外部の低電圧電源、または接地電圧が
印加されている。
そして前記第3グリツド7及び前記第5グリツ
ド9の周縁部にはそれぞれ前記第1の電極25及
び第2の電極27の側面を略覆うようにシールド
構体46,47が突出されている。
前述した構造を有する本発明の一実施例の特徴
は第1の電極25及び第2の電極27が特に電源
に接続されてなく、所謂“浮いている”状態にな
つており、こられ2個の電極25,27にそれぞ
れ対設した第3グリツド7第3の電極26及び第
5グリツド9間に形成されるコンデンサにより、
その電位が決定されるので、前記2個の電極2
5,27の周囲の構造物の電位が変化するとそれ
に伴つて第1の電極25及び第2の電極27の電
位が変化することになり即ち不安定状態となる。
特に図に示すように一般にカラー受像管の電子銃
は、前記カラー受像管の細いネツク部48に内装
されているため、このネツク部48内面の電位の
影響を受けやすい。例えば図の如くネツク部48
内面には導電膜49が塗布されており、この導電
膜49の影響により前記第1の電極25及び第2
の電極27からなる第2集束電極附近のネツク部
48内面の電位が上昇する。
前記ネツク部48内面の電位の上昇は或る時間
を経過すれば安定するが、この安定迄の時間はカ
ラー受像管の形状、その他により差異があり一般
には10分から長い場合には30分以上の時間を必要
とすることがある。
即ち先願の電子銃に於てはこのネツク部48内
面の電位が上昇すると等価的には第3図に示した
等価回路に於てコンデンサC1,C2に蓄積するチ
ヤージ量が変化することになり結果的には前記等
価回路で計算された附与電圧とは異なつてくるの
で不安定現象が表われたが、本発明の電子銃の如
くシールド構体46,47を設けることにより前
記ネツク部内面の電位の変化を前記第1の電極2
5及び第2の電極27が受けない様な構造として
ある。
前述の様に前記第1の電極25及び第2の電極
27の側面を略覆うようにシールド構体46,4
7を設けることにより、ネツク部48内面の電位
変化の影響が皆無となり、カラー受像管の動作ス
タート時と長時間動作後に於ても、前記第1の電
極25及び第2の電極27に与えられる電位が常
に一定となり極めて集束特性のよい電子銃を得る
ことが出来た。
前記実施例では第3グリツド7及び第5グリツ
ド9よりシールド構体を延長させたが、これは第
4グリツド8の第3の電極26の周縁部に、前記
第1の電極25及び第2の電極27の側壁部を略
覆うようにシールド構体を形成しても前記実施例
と同様な効果が得られることは説明する迄もな
い。 DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electron gun that emits a plurality of electron beams, and more particularly to a structure of an electron gun that can focus the electron beams on a target with extremely high precision. For example, in a normal color picture tube equipped with an electron gun that emits a plurality of electron beams, each of the electron beams passes through a respective electron lens and is deposited on the inner surface of the face plate of the color picture tube. The light is focused on a predetermined phosphor layer of a target consisting of dot-shaped or band-shaped phosphor layers that emit red, green, and blue colors.
In this case, the electron lens is generally formed by an electrostatic field, and the electron beam is focused while passing through the electrostatic field. The electrostatic field is formed between at least two opposing electrodes that are arranged perpendicular to the path of the electron beam and have an aperture through which the electron beam passes, and the characteristics of the electron lens created by this electrostatic field are normal. It can be changed depending on the voltage and distance applied between the opposing electrodes, the size of the aperture through which the electron beam passes, etc. In addition, it is said that the performance of an electron gun is better as the magnification and spherical aberration of the electron lens are smaller. Therefore, it is necessary to use an electron lens with a long focal length, but the most effective method is to use a voltage between electrodes. In general, the stem pins installed in the base of the color picture tube must be within a range that does not cause mutual discharge, and the dimensions of the aperture through which the electron beam passes must be such that the inner diameter of the neck of the color picture tube is Since it is constrained by other electrical conditions, it is not possible to design it arbitrarily large, and furthermore, increasing the distance between the opposing electrodes will reduce the stray electric field generated on the inner wall of the network and the This is also unsuitable since the properties of the electron lens are affected by the undesired electric field of the electron lens. In any case, the design of the electronic lens is constrained by the physical conditions determined by the design of the color picture tube. This is especially true in the case of color picture tubes, which require multiple electron beams, so the above-mentioned limitations are particularly severe. A general trend to circumvent the various constraints mentioned above is to combine electrode voltages and electrode numbers within permissible ranges to create long focal length electron lenses. For example, JP-A-51-76072
An example of this is the electron gun described in Japanese Patent Laid-Open No. 51-77061. As seen in these examples, methods of combining electrode voltages and types of electrodes generally complicate the structure of the electron gun, or require additional voltages to be applied in order to form an electron lens. , which usually impairs economic efficiency. Generally, in order to improve the performance of an electronic lens, the voltage to be applied must be increased, including the example mentioned above. In order to ensure the reliability of a television receiver equipped with a picture tube, special measures must be taken, which further reduces economic efficiency. In order to overcome the above-mentioned drawbacks, the inventor first applied for an electron gun whose electron lens was designed to focus at a high voltage, but the voltage externally applied to the color picture tube was lower than that. Next, Figure 1 a, b, Figure 2 and 3
The structure and equivalent circuit will be explained with reference to figures. The basic type of the electron gun shown in the figure is a well-known unipontential in-line electron gun, and the electron gun 1 consists of a plurality of electrodes and a plurality of glass support rods 10 that support them. The electrodes are three cathodes 2, 3, 4, a first grid 5, a second grid 6, a first or third focusing grid 7.
A second or fourth focusing grid 8 and a second or fifth focusing grid 9 are attached to the glass rod 10 in this order. the three cathodes 2;
Reference numerals 3 and 4 emit electron beams along the paths of three beams on the same plane, and the first grid 5 and the second grid 6 are flat electrodes arranged close to each other, each aligned with each electron beam path. The third grid 2 has three openings arranged close to the second grid 6 and has two cups 2 joined at their open ends.
0 and 21, and the closed ends of the cups 21 and 21 have three holes aligned with each electron beam path, respectively.
Electron beam apertures are provided. Openings 17, 18, 1 of the first cup 20
9 has a larger diameter than the opening of the second grid 6, and the openings 22, 23, 24 of the second cup 21 have a diameter larger than that of the opening of the second grid 6.
The opening of the cup 20 is larger than that of the cup 20 shown in FIG. Further, the fourth grid 8 is made up of at least three auxiliary electrodes, the first electrode 25 and the second electrode 27 are each made up of two cup-shaped electrodes joined together, and each of the three auxiliary electrodes is aligned with each electron beam path. An opening is provided. This first electrode 25 and the second
The electrodes 27 are electrically connected and have the same potential. The first electrode 25 and the second electrode 27 are spaced apart from each other in the electron beam path direction, and a third plate-shaped electrode 26 (hereinafter simply a third
) is arranged, and this third electrode 26
There are also three apertures aligned with each electron beam path. The fifth grid 9 is the third grid
7 and the fourth grid 8 by a distance approximately equal to the distance between the fourth grid 8 and the fourth grid 8 ;
At least 3 electron beams aligned with each of the 3 electron beam paths
It consists of a cup-shaped electrode provided with apertures. The three openings 36 of this fifth grid 9,
Among the holes 37 and 38, the central opening 37 is aligned with the openings from the first grid 5 to the fourth grid 8 , but the openings 36 and 38 on both sides are outside the central opening 37, respectively. It is slightly deviated towards the other side. Further attached to the fifth grid 9 is a converge escape cap 42 having a bottomed cylindrical shape and having three openings at its bottom substantially aligned with each electron beam path. A valve spacer 45 made of three metal strips projecting outward is attached to the open end of the converge encup 42. In the electron gun having such a structure, the third grid 7 and the fifth grid 9 are connected, an anode voltage is applied through the valve spacer 45, and the fourth grid is connected to the third grid 7 and the fifth grid 9.
Connecting the first electrode 25 and second electrode 27 of 8 ,
Especially considering the case where no voltage is applied and the third electrode 26 is grounded, for example, the first electrode 25,
The second electrode 27 has a distance G 1 between the facing surfaces of the third grid 7 and the first electrode 25 and a distance G 1 between the facing surfaces of the first electrode 25 and the third electrode 26.
G 2 and capacitors C 1 and C 2 approximately determined by
The potential generated by this will be applied as a focusing voltage. In this case, the third electrode 26 is preferably designed so as not to significantly influence the focusing voltage of the electron gun. That is, a voltage of 0 volts is applied to the third electrode 26, E=25 KV is applied to the anodes, that is, the third grid 7 and the fifth grid 9, and the voltage of the first electrode 25 and the second electrode 27 of the fourth grid 8 is applied. If e 2 is 9KV,
As is clear from the equivalent circuit in Figure 3, G 1 /G 2
= 1/0.6, but
Here, the gap ratio of G 1 /G 2 changes depending on the shape of the opposing part of each electrode, so generally speaking, G 1 /G 2 =
It is not 1/0.6. In other words, the electron gun having the above-mentioned structure is excellent in that it has the desired performance as the electron gun mentioned above despite the low voltage applied from the outside, but the focusing electrode, i.e. First electrode 25
and that the potential of the second electrode 27 is unstable;
That is, there is a drawback that the voltages to be applied to the first electrode 25 and the second electrode 27 at the start of operation of the color picture tube and after long-time operation are likely to change. The present invention has been made in view of the above drawbacks, and
The present invention relates to a structure of an electron gun that eliminates the problems of the previous application and can obtain a constant focused voltage from the start of operation of a color picture tube until after a long period of operation. Next, one embodiment of the present invention will be explained with reference to FIG. In the figure, the same reference numerals as those in the previous application indicate the same parts, and no particular explanation will be given. i.e. the first focusing grid, i.e. the third grid 7.
and the third focusing grid, that is, the fifth grid 9, are connected and an anode voltage is applied, and the fourth grid 8
The first electrode 25 and the second electrode 27 are connected to each other, and no voltage is applied to the third electrode 26 inserted between the first electrode 25 and the second electrode 27. is connected to an external low voltage power supply or ground voltage. Shield structures 46 and 47 are protruded from the peripheral edges of the third grid 7 and the fifth grid 9 so as to substantially cover the side surfaces of the first electrode 25 and second electrode 27, respectively. A feature of the embodiment of the present invention having the above-described structure is that the first electrode 25 and the second electrode 27 are not particularly connected to a power source and are in a so-called "floating" state. By the capacitor formed between the third electrode 26 of the third grid 7 and the fifth grid 9, which are arranged opposite to the electrodes 25 and 27, respectively,
Since the potential is determined, the two electrodes 2
When the potentials of the structures around the electrodes 5 and 27 change, the potentials of the first electrode 25 and the second electrode 27 change accordingly, ie, become unstable.
In particular, as shown in the figure, the electron gun of a color picture tube is generally housed in a thin neck portion 48 of the color picture tube, and therefore is susceptible to the influence of the potential on the inner surface of this neck portion 48. For example, as shown in the figure, the network part 48
A conductive film 49 is coated on the inner surface, and due to the influence of this conductive film 49, the first electrode 25 and the second electrode
The potential on the inner surface of the network portion 48 near the second focusing electrode consisting of the electrode 27 increases. The rise in potential on the inner surface of the network portion 48 stabilizes after a certain period of time, but the time it takes to stabilize varies depending on the shape of the color picture tube and other factors, and generally takes 10 minutes or more than 30 minutes. Sometimes it takes time. That is, in the electron gun of the prior application, when the potential on the inner surface of the network portion 48 rises, the amount of charge accumulated in the capacitors C 1 and C 2 changes in the equivalent circuit shown in FIG. 3. However, by providing the shield structures 46 and 47 as in the electron gun of the present invention, the applied voltage differs from the applied voltage calculated using the equivalent circuit described above, so that the applied voltage is different from that calculated using the equivalent circuit. Changes in the potential on the inner surface of the first electrode 2
5 and the second electrode 27 are not received. As described above, the shield structures 46 and 4 are installed so as to substantially cover the side surfaces of the first electrode 25 and the second electrode 27.
By providing 7, there is no influence of potential changes on the inner surface of the network portion 48, and even at the start of operation of the color picture tube and after a long period of operation, the potential change applied to the first electrode 25 and the second electrode 27 is completely eliminated. We were able to obtain an electron gun with extremely good focusing characteristics because the potential was always constant. In the above embodiment, the shield structure is extended from the third grid 7 and the fifth grid 9 , but this is because the first electrode 25 and the second electrode It goes without saying that even if the shield structure is formed so as to substantially cover the side wall portion of 27, the same effect as in the embodiment described above can be obtained.
第1図は先願の電子銃の側面図及び平面図、第
2図は第1図の断面図、第3図は第2図の主要部
分の原理を説明するための等価回路、第4図は本
発明の電子銃の一実施例及びネツク部を示す断面
図である。
1……電子銃、2,3,4……陰極、5……第
1グリツド、6……第2グリツド、7……第3グ
リツド(第1集束電極)、8……第4グリツド
(第2集束電極)、9……第5グリツド(第3集束
電極)、46,47……シールド構体、48……
ネツク部、49……導電膜。
Figure 1 is a side view and plan view of the electron gun of the earlier application, Figure 2 is a sectional view of Figure 1, Figure 3 is an equivalent circuit for explaining the principle of the main parts of Figure 2, and Figure 4. 1 is a sectional view showing an embodiment of the electron gun of the present invention and a neck portion. 1 ... Electron gun, 2, 3, 4... Cathode, 5... First grid, 6... Second grid, 7 ... Third grid (first focusing electrode), 8 ... Fourth grid (first focusing electrode). 2 focusing electrode), 9... Fifth grid (third focusing electrode), 46, 47... Shield structure, 48...
Network portion, 49... conductive film.
Claims (1)
第5グリツドを有し、前記第4グリツドがそれぞ
れ前記第3グリツドと前記第5グリツドにそれぞ
れ対設し互いに電気的に接続された第1の電極と
第2の電極及び前記第1の電極と第2の電極間に
挿入された第3の電極よりなり、前記第3グリツ
ド、第1の電極、第3の電極、第2の電極及び第
5グリツドとの間にそれぞれ形成されるコンデン
サを介して前記第1の電極及び第2の電極に電位
が附与されるようにした電子銃に於て、前記第1
の電極及び前記第2の電極の側面を略覆うような
シールド構体を配設したことを特徴とする電子
銃。 2 シールド構体が第3グリツド及び第5グリツ
ドの周縁部から突出形成されていることを特徴と
する特許請求の範囲第1項記載の電子銃。 3 シールド構体が第3電極の周縁部から第3グ
リツド及び第5グリツド方向に突出形成されてい
ることを特徴とする特許請求の範囲第1項記載の
電子銃。[Scope of Claims] 1 At least a third grid, a fourth grid, and a fifth grid, wherein the fourth grid is provided opposite to the third grid and the fifth grid, respectively, and electrically connected to each other. It consists of a first electrode, a second electrode, and a third electrode inserted between the first electrode and the second electrode, and the third grid, the first electrode, the third electrode, and the second electrode. In the electron gun, a potential is applied to the first electrode and the second electrode via capacitors formed between the electrode and the fifth grid, respectively.
An electron gun characterized in that a shield structure is disposed to substantially cover side surfaces of the electrode and the second electrode. 2. The electron gun according to claim 1, wherein the shield structure is formed to protrude from the peripheral edges of the third grid and the fifth grid. 3. The electron gun according to claim 1, wherein the shield structure is formed to protrude from the peripheral edge of the third electrode in the direction of the third grid and the fifth grid.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5200778A JPS54144173A (en) | 1978-04-28 | 1978-04-28 | Electron gun |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5200778A JPS54144173A (en) | 1978-04-28 | 1978-04-28 | Electron gun |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS54144173A JPS54144173A (en) | 1979-11-10 |
| JPS6243302B2 true JPS6243302B2 (en) | 1987-09-12 |
Family
ID=12902757
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5200778A Granted JPS54144173A (en) | 1978-04-28 | 1978-04-28 | Electron gun |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS54144173A (en) |
-
1978
- 1978-04-28 JP JP5200778A patent/JPS54144173A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS54144173A (en) | 1979-11-10 |
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