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JPH0146986B2 - - Google Patents
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JPH0146986B2 - - Google Patents

Info

Publication number
JPH0146986B2
JPH0146986B2 JP55000418A JP41880A JPH0146986B2 JP H0146986 B2 JPH0146986 B2 JP H0146986B2 JP 55000418 A JP55000418 A JP 55000418A JP 41880 A JP41880 A JP 41880A JP H0146986 B2 JPH0146986 B2 JP H0146986B2
Authority
JP
Japan
Prior art keywords
electrode
electrodes
focusing
anode
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
Application number
JP55000418A
Other languages
Japanese (ja)
Other versions
JPS5697947A (en
Inventor
Kazuaki Naiki
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
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP41880A priority Critical patent/JPS5697947A/en
Publication of JPS5697947A publication Critical patent/JPS5697947A/en
Publication of JPH0146986B2 publication Critical patent/JPH0146986B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/46Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
    • H01J29/58Arrangements for focusing or reflecting ray or beam
    • H01J29/62Electrostatic lenses
    • H01J29/622Electrostatic lenses producing fields exhibiting symmetry of revolution
    • H01J29/624Electrostatic lenses producing fields exhibiting symmetry of revolution co-operating with or closely associated to an electron gun

Description

【発明の詳細な説明】 本発明は複数の電子ビームを発生するカラー陰
極線管の多電子銃電極構体、特に電気的、構造的
に共通で各電子ビーム通路には実質的に個別、或
いは共通の電子レンズを形成する一体化電極を備
えた電子銃電極構体に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a multi-electron gun electrode structure for a color cathode ray tube that generates a plurality of electron beams. The present invention relates to an electron gun electrode assembly with an integrated electrode forming an electron lens.

電子銃電極構体の組立作業の簡易化、組立精度
の向上、或いはカラー陰極線管の電子銃が封止さ
れる硝子外囲器頚部の径小化に伴う電子銃電極構
体の占有体積の縮小化を実現する手段として電気
的、構造的に共通で各電子ビーム通路には実質的
に個別、或いは共通の電子レンズを形成する一体
化電極を備えた電子銃電極構体が一般に用いられ
ている。更に電子ビームに対する電子銃主電子レ
ンズの集束特性を大幅に改善する手段として、一
つの主電子レンズによらず複数の電子レンズを組
合せた多段集束型電子レンズを備えた電子銃電極
構体が用いられているが、その電極構成によつて
は電極の軸方向長さが対向電極間隙と同程度、或
いはそれ以下となる電極があり、その電極の熱容
量は他の電極と比べて著しく小さくなり、又電極
支持子間の相互距離も対向電極間隙と同程度なる
ことがある。電子銃の動作時には前記電極間に異
つた高電圧が印加され、各対向電極間に大きな電
位差が生じるため電極相互間の耐電圧特性は良好
でなければならない。従がつて陰極線管製造工程
中、上述の高電位差の生じる電極間の耐電圧特性
を向上させるために高電圧処理が行われるが、複
数の電極間に大きな熱容量の差があつたり、電極
支持体間の相互距離に大きな差があると、電極間
を十分高電圧処理が出来ず、電極相互間の耐電圧
特性は著しく劣化する。
Simplify the assembly work of the electron gun electrode assembly, improve assembly accuracy, or reduce the volume occupied by the electron gun electrode assembly due to the reduction in the diameter of the neck of the glass envelope in which the electron gun of a color cathode ray tube is sealed. As a means of achieving this, an electron gun electrode assembly is generally used which is electrically and structurally common and includes an integrated electrode for each electron beam path forming a substantially separate or common electron lens. Furthermore, as a means to significantly improve the focusing characteristics of the main electron lens of the electron gun for the electron beam, an electron gun electrode assembly is used which is equipped with a multi-stage focusing electron lens that combines multiple electron lenses instead of just one main electron lens. However, depending on the electrode configuration, there are some electrodes whose axial length is the same as or less than the gap between opposing electrodes, and the heat capacity of these electrodes is significantly smaller than that of other electrodes. The mutual distance between electrode supports may also be comparable to the gap between opposing electrodes. During operation of the electron gun, different high voltages are applied between the electrodes, and a large potential difference occurs between each opposing electrode, so the voltage resistance characteristics between the electrodes must be good. Therefore, during the cathode ray tube manufacturing process, high voltage treatment is performed in order to improve the withstand voltage characteristics between the electrodes where the above-mentioned high potential difference occurs, but there is a large difference in heat capacity between multiple electrodes, and the electrode support If there is a large difference in the mutual distance between the electrodes, a sufficiently high voltage cannot be applied between the electrodes, and the withstand voltage characteristics between the electrodes will deteriorate significantly.

従来用いられている多段集束型電子レンズを備
えた電子銃電極構体の一つについて第1図〜第3
図に従がつて説明する。第1図及び第2図は従来
用いられている同一平面内に互に電気的に絶縁さ
れて等間隔距離を保つて陰極が配列されたインラ
イン型で、主電子レンズが3個のバイ・ポテンシ
ヤル・フオーカス電子レンズを積重ねた多段集束
型電子レンズ方式を採る電子銃電極構体1の夫々
正面図及び側面図、第3図は第1図に示すA−A
断面を示す。
Figures 1 to 3 show one of the conventionally used electron gun electrode structures equipped with multistage focusing electron lenses.
This will be explained according to the diagram. Figures 1 and 2 show a conventional in-line type in which cathodes are arranged on the same plane, electrically insulated from each other and equally spaced apart, and the main electron lens is a bipotential type with three main electron lenses.・A front view and a side view of the electron gun electrode structure 1 which adopts a multi-stage focusing electron lens system in which focus electron lenses are stacked, respectively, and FIG. 3 is A-A shown in FIG. 1.
A cross section is shown.

電子銃電極構体1は同一平面内に互に絶縁され
て等間隔距離を保つて一列に配列された陰極構体
10と、これに対向して電子ビーム進行方向に順
次配置される電気的に共通な制御電極であるG1
電極11、及び陰極より射出された熱電子ビーム
の加速電極であるG2電極12、電気的、構造的
に共通で各電子ビーム通路には実質的に独立した
電子レンズを形成する一体化電極からなる第1集
束電極であるG3電極13、第1陽極電極である
G4電極14、第2集束電極であるG5電極15、
第2陽極電極であるG6電極16で構成されてい
る。
The electron gun electrode assembly 1 includes cathode assemblies 10 which are insulated from each other and arranged in a line at equal intervals in the same plane, and electrically common cathode assemblies 10 which are arranged in sequence in the electron beam traveling direction in opposition to these cathode assemblies 10. G1, the control electrode
The electrode 11 and the G2 electrode 12, which is an accelerating electrode for the thermionic beam emitted from the cathode, are electrically and structurally common, and each electron beam path is composed of an integrated electrode that forms a substantially independent electron lens. G3 electrode 13 is the first focusing electrode, and the first anode electrode
G4 electrode 14, G5 electrode 15 which is a second focusing electrode,
It is composed of a G6 electrode 16 which is a second anode electrode.

各電極は絶縁物支持杆19との融着強度を高め
るために複数の切欠部18Aを先端に設けた支持
子18を持ち、支持子18の切欠部18Aを二本
の直方柱状絶縁支持杆19へ埋込んで融着するこ
とにより各電極間隔が所定寸法に保持固定されて
いる。G4電極14とG6電極16は給電線17A
により同電位となるように接続され、図示しない
が電子銃電極構体1が封止される陰極線管硝子外
囲器漏斗状部に配設された陽極端子に接続された
内部導電性被膜から20〜30KV程度の高電圧の陽
極電圧が供給され、G3電極13とG5電極15は
給電線17Bにより同電位とされ、図示されてい
ないが電子銃電極構体1が支持固定されるステム
の給電ピンから陽極電圧の20〜40%程度の集束電
圧が供給され、他の電極もステムの給電ピンより
所定電圧が供給される様に互にステムの給電ピン
に接続される。陰極10より放射された電子ビー
ムはG1電極11とG2電極12付近に形成される
クロス・オーバ点より発散され、G2電極12と
G3電極13間に形成されるブリ・フオーカス・
レンズで予備集束された後、G3電極13とG4電
極14、G4電極14とG5電極15、G5電極15
とG6電極16の電極間隙に形成される主フオー
カス・レンズとなる夫々独立した3個のバイ・ポ
テンシヤル型レンズで三段に順次集束され、螢光
面上で最小のビーム・スポツト断面積を持つよう
に集束電極であるG3電極13及びG5電極15に
印加される集束電圧が調整される。プリ・フオー
カス電子レンズで予備集束された電子ビームは3
個の主フオーカス・レンズで三段に集束されるた
め、主フオーカス・レンズは従来用いられている
電子銃に於ける1個からなる主フオーカス・レン
ズより夫々のレンズ強度は弱く出来る。従がつて
3個の主電子レンズで徐々に電子ビームを集束出
来て、主電子レンズ系の球面収差は極めて小さく
なり、陰極線管動作時の高輝度画面となる大ビー
ム電流時に於ても電子ビーム束は各主電子レンズ
の収差の小さい中心部を通過することになり、細
く集束されたビーム束が得られ、螢光面上には高
輝度画面であつても高解像度の受像画像が得られ
る。
Each electrode has a supporter 18 having a plurality of notches 18A at its tip to increase the strength of the fusion bond with the insulator support rod 19. By embedding and fusing the electrodes into each other, the distance between each electrode is maintained and fixed at a predetermined dimension. G4 electrode 14 and G6 electrode 16 are power supply lines 17A
Although not shown, the internal conductive coating is connected to the anode terminal disposed in the funnel-shaped part of the cathode ray tube glass envelope in which the electron gun electrode structure 1 is sealed. A high anode voltage of about 30 KV is supplied, and the G3 electrode 13 and the G5 electrode 15 are brought to the same potential by the power supply line 17B. Although not shown, the anode is connected to the power supply pin of the stem on which the electron gun electrode assembly 1 is supported and fixed. A focused voltage of about 20 to 40% of the voltage is supplied, and the other electrodes are also connected to the power supply pin of the stem so that a predetermined voltage is supplied from the power supply pin of the stem. The electron beam emitted from the cathode 10 is diverged from a crossover point formed near the G1 electrode 11 and the G2 electrode 12, and is separated from the G2 electrode 12.
Buri focus formed between G3 electrodes 13
After pre-focusing with the lens, G3 electrode 13 and G4 electrode 14, G4 electrode 14 and G5 electrode 15, G5 electrode 15
The beam is sequentially focused in three stages by three independent bipotential type lenses, which are formed in the gap between the G6 electrode 16 and the main focus lens, and has the smallest beam spot cross-sectional area on the fluorescent surface. The focusing voltages applied to the G3 electrode 13 and the G5 electrode 15, which are focusing electrodes, are adjusted in this manner. The electron beam pre-focused by the pre-focus electron lens is 3
Since the main focus lenses are focused in three stages, the strength of each main focus lens can be weaker than that of a single main focus lens in a conventional electron gun. Therefore, the three main electron lenses can gradually focus the electron beam, and the spherical aberration of the main electron lens system becomes extremely small, so that the electron beam can be focused even when the beam current is large, which is the high brightness screen during cathode ray tube operation. The beam passes through the center of each main electron lens with small aberrations, resulting in a narrowly focused beam, and a high-resolution received image can be obtained on the fluorescent surface even on a high-brightness screen. .

ここに主電子レンズの一部を構成するG5電極
15を例に採り詳細にその電極支持構造を見る
と、第3図に電子ビーム進行方向に垂直な断面で
示す様に一直線上に整列して中央及び両外側電子
ビーム透過孔として穿設された三つの開孔15
R,15G,15Bの配列方向に長く、配列方向
の直角方向に短い略々長方形、或いは長円形状を
呈した閉塞端面及び筒側部とを持つた閉塞筒状体
であり、開放端には筒側部に連続して直角に張出
された鍔状縁15Aが一体に形成され、長辺側の
鍔状縁15Aには絶縁物支持杆19との融着強度
を高めるために複数の切欠部18Aを先端に設け
て電極支持子18を構成し、二つの閉塞筒状体電
極が鍔状縁15Aで夫々重ね合せられている。
Taking the G5 electrode 15 that constitutes a part of the main electron lens as an example, and looking at its electrode support structure in detail, we can see that the electrodes are aligned in a straight line as shown in the cross section perpendicular to the electron beam traveling direction in Figure 3. Three apertures 15 bored as center and both outer electron beam transmission holes
It is a closed cylindrical body that has a closed end face and a cylinder side part that is long in the arrangement direction of R, 15G, and 15B and has a substantially rectangular or elliptical shape that is short in the direction perpendicular to the arrangement direction, and the open end has a closed end face and a cylinder side part. A flanged edge 15A extending at right angles to the cylinder side is integrally formed, and the flanged edge 15A on the long side has a plurality of notches in order to increase the strength of the welding with the insulator support rod 19. A portion 18A is provided at the tip to constitute an electrode supporter 18, and two closed cylindrical body electrodes are overlapped with each other at a flanged edge 15A.

上述の様にG4電極14とG6電極16に高電圧
の陽極電圧が、G3電極13とG5電極15には集
束電圧として陽極電圧の20〜40%程度の中高電圧
が印加される。即ちG3電極13乃至G6電極16
迄の電極間には高電圧の陽極電圧と中高電圧の集
束電圧とが周期的に印加されて、G3電極13と
G4電極14、G4電極14とG5電極15及びG5
電極15とG6電極16間には大きな電位差を生
じるため、対向する電極相互間隔及び絶縁物支持
杆19に埋設される支持子相互間隔の大きさは耐
電圧特性に大きく影響する。G3電極13とG4電
極14、G4電極14とG5電極15及びG5電極1
5とG6電極16の各電極相互間隔a1a2a3は耐電
圧特性上大きい程よいが、余り大きいと外部電界
の侵入の影響を受け、電子ビーム通過中の電子ビ
ーム径路を不所望に曲げてしまうため、この影響
を受けない大きさで、且つ等しい大きさに選定さ
れている。一方G3電極13、G4電極14、G5電
極15、G6電極16の各電極支持子18相互間
の耐電圧特性は絶縁物支持杆19の組成による固
着抵抗値及び表面状態等による表面抵抗値に応じ
て流れる微小漏洩電流で決まるため、G3電極1
3とG4電極14、G4電極14とG5電極15、
G5電極15とG6電極16の電極支持子18間距
離A1A2A3は可能の限り大きくして、絶縁物支持
杆19に沿つた最短漏洩電流径路は大きいことが
望ましいが、これはフオーカス特性から決まる各
電極の軸方向長さ、及び電極相互間隔a1a2a3で決
定される。通常上記電極間隔a1a2a3は0.8〜1.5mm
程度に選定され、対向電極面の表面状態は電子銃
電極構体及び陰極線管の製造工程に於ける処理で
耐電圧上問題ない清浄な表面とすることが可能で
あり、且つ陰極線管は高真空中で動作することを
考慮すれば50〜80KV程度の耐電圧特性を有する
ことになり、電極間隔の大きさは耐電圧特性上余
り問題ではなく、寧ろ電極間の耐電圧特性を決定
する主要因は絶縁物支持杆19表面に沿つた電極
支持子間距離であると云える。
As described above, a high anode voltage is applied to the G4 electrode 14 and the G6 electrode 16, and a medium-high voltage of about 20 to 40% of the anode voltage is applied to the G3 electrode 13 and the G5 electrode 15 as a focusing voltage. That is, G3 electrode 13 to G6 electrode 16
A high voltage anode voltage and a medium-high voltage focusing voltage are periodically applied between the G3 electrode 13 and the G3 electrode 13.
G4 electrode 14, G4 electrode 14 and G5 electrode 15 and G5
Since a large potential difference is generated between the electrode 15 and the G6 electrode 16, the distance between the opposing electrodes and the distance between the supports embedded in the insulating support rod 19 greatly affect withstand voltage characteristics. G3 electrode 13 and G4 electrode 14, G4 electrode 14 and G5 electrode 15, and G5 electrode 1
The larger the inter-electrode spacing a1a2a3 of the 5 and G6 electrodes 16, the better from the viewpoint of withstand voltage characteristics, but if it is too large, the electron beam path will be undesirably bent due to the influence of external electric field penetration. Therefore, the sizes are selected to be equal and not affected by this effect. On the other hand, the withstand voltage characteristics between the electrode supports 18 of the G3 electrode 13, G4 electrode 14, G5 electrode 15, and G6 electrode 16 depend on the fixed resistance value due to the composition of the insulator support rod 19 and the surface resistance value due to the surface condition, etc. G3 electrode 1
3 and G4 electrode 14, G4 electrode 14 and G5 electrode 15,
It is desirable that the distance A 1 A 2 A 3 between the electrode supports 18 of the G5 electrode 15 and the G6 electrode 16 be as large as possible, so that the shortest leakage current path along the insulator support rod 19 is large. It is determined by the axial length of each electrode determined from the characteristics and the mutual electrode spacing a 1 a 2 a 3 . Normally the above electrode spacing a 1 a 2 a 3 is 0.8 to 1.5 mm
The surface condition of the counter electrode surface can be made to be a clean surface with no problem with withstand voltage during the manufacturing process of the electron gun electrode structure and cathode ray tube, and the cathode ray tube can be used in a high vacuum. Considering that it operates at 50 to 80 KV, it has a withstand voltage characteristic of about 50 to 80 KV, and the size of the electrode spacing is not a big problem in terms of withstand voltage characteristics.In fact, the main factor that determines the withstand voltage characteristics between the electrodes is It can be said that this is the distance between the electrode supports along the surface of the insulator support rod 19.

然るに従来はG3電極13、G4電極14、G5電
極15は必要とする軸方向長さを二等分した長さ
を持つた二つの閉塞筒状体電極13-1,13-2
14-1,14-2,15-1,15-2をその鍔状縁を
重ね合せて夫々形成されていたため、第2図に示
す様にG3電極13、G4電極14、G5電極15、
G6電極16の各電極支持子18間隔A1A2A3は不
等長となり、特にフオーカス特性から決る電極構
成によつては、或る電極の軸方向長さが他の電極
のそれより著しく短くなり(第2図の場合では
G4電極14)、この電極に隣接した電極の夫々の
電極支持子間隔A1A2は他の間隔A3に比べて短く
なり、絶縁物支持杆19に沿つた電極支持子18
間に形成される最短漏洩電流経路に長短が生じ
る。この内の最小径路が電極間に印加される高電
圧に対する耐電圧に不十分の長さであつたり、或
いは陰極線管製造工程中、上述の高電位差の生じ
る電極間の耐電圧特性を向上させるため、実際に
使用される陽極定格電圧の数倍相当の高電圧を印
加して、電極表面の微小突起や、汚れ等を除去す
る高電圧処理工程があるが、この時電極支持子間
の最短漏洩電流経路中の最小径路に高負荷がかか
り、漏洩電流がこの間に集中する為余り大きな高
電圧を印加して高電圧処理が出来ず、耐電圧特性
は良好でなくなる。
However, conventionally, the G3 electrode 13, the G4 electrode 14, and the G5 electrode 15 are two closed cylindrical electrodes 13 -1 , 13 -2 , whose length is equal to the required axial length.
14 -1 , 14 -2 , 15 -1 , 15 -2 were formed by overlapping their brim-like edges, so as shown in FIG. 2, G3 electrode 13, G4 electrode 14, G5 electrode 15,
The spacing A 1 A 2 A 3 of each electrode supporter 18 of the G6 electrode 16 has unequal lengths, and depending on the electrode configuration determined by the focus characteristics, the axial length of one electrode may be significantly greater than that of another electrode. becomes shorter (in the case of Figure 2)
G4 electrode 14), the distance A 1 A 2 between the electrode supports of the electrode adjacent to this electrode is shorter than the other distance A 3 , and the electrode support 18 along the insulator support rod 19
The shortest leakage current path formed between the two is long or short. The length of the shortest path is insufficient to withstand the high voltage applied between the electrodes, or to improve the withstand voltage characteristics between the electrodes where the above-mentioned high potential difference occurs during the cathode ray tube manufacturing process. There is a high-voltage treatment process in which a high voltage equivalent to several times the rated voltage of the anode actually used is applied to remove minute protrusions and dirt on the electrode surface. A high load is applied to the smallest path in the current path, and leakage current is concentrated during this period, so too much high voltage is applied and high voltage processing is not possible, resulting in poor withstand voltage characteristics.

更に上述の高電圧処理工程では陽極電極である
G6電極16、G4電極14に陽極定格電圧の数倍
の高電圧を印加し、これ以外の他電極、即ち集束
電極であるG5電極15、G3電極13及びG2電極
12、G1電極11、陰極10は接地電位に保た
れている。主電子レンズ電極相互間隔a1a2a3は通
常0.8〜1.5mm程度で、高電圧処理電圧は50〜
80KV程度であり、従がつて主電子レンズ電極相
互間には50〜100MV/mの強電界がかかること
になり、いわゆる冷陰極放出作用により高電位電
極であるG6電極16、G4電極14から接地電位
であるG5電極15、G3電極13に向う冷陰極放
出電流が流入する。換言すれば第2図中矢印Bで
示す様に冷陰極放出電子が接地電位にあるG5電
極15、G3電極13から高電位にあるG6電極1
6、G4電極14へ流入することになり、しかも
電子は強電界で高速度に加速され、G6電極16、
G4電極14の接地電位にある電極に対向する電
極表面に激突し、電子の運動エネルギーは熱に変
換されて、その熱で高電圧処理期間中電極は加熱
され続け、G6電極16、G4電極14の電極表面
温度は急激に上昇していく。特に第2図中矢印B
で示す様に高電圧処理工程中、接地電位にある
G3電極13、G5電極15にはさまれたG4電極1
4にはG3電極13とG5電極15から電子が激突
し、両面が加熱されることになり、片面だけ加熱
されるG6電極16より2倍加熱される。更に主
電子レンズ電極構成の設計寸法から決定される電
極の軸方向長さが、他の電極や電極間隔に対して
著しく短い第2図に示すG4電極14は他の電極
と比べて熱容量も著しく小さいため、激突する電
子により赤熱するに至る迄加熱され、同時に電極
支持部18も赤熱され、その局部的熱で絶縁物支
持杆19を局部的に歪ませて、その結果絶縁物支
持杆19に割目を形成したり、或いはこれを破壊
する迄に至り、電子銃電極構体1を機械的、電気
的に不良にしてしまう。従がつて高電圧処理の条
件は絶縁物支持杆19の破壊防止を考慮したG4
電極14に対向するG3電極13、G5電極15の
電極間処理条件に制限され、そのために耐電圧品
位は不十分であつた。
Furthermore, in the high voltage treatment process mentioned above, the anode electrode
A high voltage several times the anode rated voltage is applied to the G6 electrode 16 and the G4 electrode 14, and the other electrodes, namely the G5 electrode 15 which is a focusing electrode, the G3 electrode 13, the G2 electrode 12, the G1 electrode 11, and the cathode 10 is held at ground potential. The main electron lens electrode mutual spacing a1a2a3 is usually about 0.8~ 1.5mm , and the high voltage processing voltage is 50~
As a result, a strong electric field of 50 to 100 MV/m is applied between the main electron lens electrodes, and due to the so-called cold cathode emission effect, the high potential electrodes G6 electrode 16 and G4 electrode 14 are grounded. A cold cathode emission current flows toward the G5 electrode 15 and the G3 electrode 13, which are at the potential. In other words, as shown by arrow B in FIG. 2, the cold cathode emitted electrons are at the ground potential at the G5 electrode 15, and from the G3 electrode 13 to the G6 electrode 1 at a high potential.
6. The electrons will flow into the G4 electrode 14, and will be accelerated at high speed by a strong electric field, and will flow into the G6 electrode 16.
The kinetic energy of the electrons collides with the surface of the electrode opposite to the electrode at ground potential of the G4 electrode 14, and the kinetic energy of the electrons is converted into heat, which continues to heat the electrode during the high voltage treatment period. The electrode surface temperature rises rapidly. In particular, arrow B in Figure 2
As shown in the figure, during the high voltage treatment process, the
G4 electrode 1 sandwiched between G3 electrode 13 and G5 electrode 15
4, electrons collide from the G3 electrode 13 and the G5 electrode 15, heating both sides, twice as much as the G6 electrode 16, which heats only one side. Furthermore, the axial length of the electrode determined from the design dimensions of the main electron lens electrode configuration is significantly shorter than other electrodes and electrode spacing, and the G4 electrode 14 shown in Figure 2 has a significantly higher heat capacity than other electrodes. Because it is small, the colliding electrons heat it up until it becomes red hot, and at the same time, the electrode support part 18 is also red hot, and the local heat causes the insulator support rod 19 to be locally distorted, and as a result, the insulator support rod 19 This may lead to the formation of cracks or breakage, resulting in the electron gun electrode assembly 1 being mechanically and electrically defective. Therefore, the conditions for high voltage treatment are G4, which takes into consideration the prevention of destruction of the insulator support rod 19.
The inter-electrode processing conditions were limited to the G3 electrode 13 and the G5 electrode 15 facing the electrode 14, and therefore the withstand voltage quality was insufficient.

本発明の目的は、上述の欠点を除去し、電極相
互間の耐電圧処理を良好に行なえて耐電圧特性の
よい電子銃電極構体を提供することである。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks and to provide an electron gun electrode structure that can perform good voltage resistance treatment between electrodes and has good voltage resistance characteristics.

本発明の陰極線管電子銃電極構体は、陰極構体
と、制御電極と、加速電極と、軸方向の長さが異
なる二つの閉塞筒状体電極をその電極支持子用の
鍔状縁で重ね合せて形成された第1集束電極、第
1陽極電極および第2集束電極と、一個の閉塞筒
状体電極よりなる第2陽極電極とがそれらの電極
支持子を絶縁物支持杆に埋設することにより、こ
の順序で配設されており、かつ第1陽極電極とそ
の両側の第1集束電極および第2集束電極との相
互の電極対向面間隔が共に第2集束電極と第2陽
極電極との相互の電極対向面間隔より大きく設定
され、さらに第1集束電極、第1陽極電極、第2
集束電極および第2陽極電極の電極支持子相互間
の最小の間隔が、軸方向の長さが等しい二つの閉
塞筒状体電極をその電極支持子用の鍔状縁で重ね
合せて第1集束電極、第1陽極電極および第2集
束電極を形成し、これらの電極対向面間隔を等し
くした場合の電極支持子相互間の最小の間隔より
大きく設定されていることを特徴とする。
The cathode ray tube electron gun electrode assembly of the present invention includes a cathode assembly, a control electrode, an accelerating electrode, and two closed cylindrical electrodes having different axial lengths, which are overlapped at the flanged edge for the electrode support. The first focusing electrode, the first anode electrode, and the second focusing electrode formed by the above electrodes, and the second anode electrode made of one closed cylindrical electrode are formed by embedding their electrode supports in an insulator support rod. , are arranged in this order, and the distance between the mutual electrode facing surfaces of the first anode electrode and the first focusing electrode and the second focusing electrode on both sides thereof is the same as that of the second focusing electrode and the second anode electrode. The distance between the electrode facing surfaces is set larger than that of the first focusing electrode, the first anode electrode, and the second electrode.
The minimum distance between the electrode supports of the focusing electrode and the second anode electrode is such that two closed cylindrical electrodes having the same length in the axial direction are overlapped at the flanged edges of the electrode supports to perform the first focusing. An electrode, a first anode electrode, and a second focusing electrode are formed, and the spacing between opposing surfaces of these electrodes is set to be larger than the minimum spacing between the electrode supports.

以下図面を参照してこの発明の一実施例を詳細
に説明する。第4図は本発明の実施例を示す電子
銃電極構体の側面図であり、説明を簡略にするた
め従来と同一のものには同一符号を付ける。
An embodiment of the present invention will be described in detail below with reference to the drawings. FIG. 4 is a side view of an electron gun electrode assembly showing an embodiment of the present invention, and in order to simplify the explanation, the same reference numerals are given to the same parts as in the conventional one.

電子銃電極構体2は同一平面内に互に絶縁され
て等間隔距離を保つて一列に配列された陰極構体
10と、これに対向して電子ビーム進行方向に順
次配置される電気的に共通な制御電極であるG1
電極11、及び陰極より射出された熱電子ビーム
の加速電極であるG2電極12、電気的、構造的
に共通で各電子ビーム通路には実質的に独立した
電子レンズを形成する一体化電極からなる第1集
束電極であるG3電極23、第1陽極電極である
第4電極24、第2集束電極であるG5電極25、
第2陽極電極であるG6電極26で従来と同様に
構成されている。各電極は絶縁支持杆19への埋
設部の形成された支持子18を持ち、各支持子1
8の埋設部を二本の絶縁物支持杆19へ埋込んで
融着することにより各電極間隔が所定寸法に保持
固定されている。従来と同様に第4電極24と
G6電極26は図示されていないが給電線で同電
位とされ、20〜30KV程度の高電圧の陽極電圧が
供給され、G3電極23とG5電極25は給電線に
より同電位とされ陽極電圧の20〜40%程の集束電
圧が供給される。
The electron gun electrode assembly 2 includes cathode assemblies 10 which are insulated from each other and arranged in a line at equal distances in the same plane, and electrically common cathode assemblies 10 which are arranged in sequence in the electron beam traveling direction in opposition to the cathode assemblies 10. G1, the control electrode
The electrode 11 and the G2 electrode 12, which is an accelerating electrode for the thermionic beam emitted from the cathode, are electrically and structurally common, and each electron beam path is composed of an integrated electrode that forms a substantially independent electron lens. G3 electrode 23 which is the first focusing electrode, fourth electrode 24 which is the first anode electrode, G5 electrode 25 which is the second focusing electrode,
It is constructed in the same manner as the conventional one with a G6 electrode 26 which is a second anode electrode. Each electrode has a support element 18 formed with a part embedded in an insulating support rod 19, and each support element 1
By embedding the embedded portions of 8 into the two insulator support rods 19 and fusing them, the distance between each electrode is maintained and fixed at a predetermined dimension. As in the past, the fourth electrode 24 and
Although not shown, the G6 electrode 26 is made to have the same potential through a power supply line, and is supplied with a high anode voltage of about 20 to 30 KV. A focusing voltage of ~40% is provided.

然るにG3電極23,G4電極24,G5電極2
5,G6電極26の軸方向の全長、電極構造は従
来と全く同様であるが、電極相互間隔が不等間隔
であり、且つ夫々の電極を構成している各組の閉
塞筒状体電極の軸方向長さは異なる長さにされて
いる。
However, G3 electrode 23, G4 electrode 24, G5 electrode 2
5. The total length in the axial direction and the electrode structure of the G6 electrode 26 are exactly the same as the conventional one, but the mutual spacing between the electrodes is unequal, and each set of closed cylindrical electrodes constituting each electrode is The axial lengths are of different lengths.

先ず電極相互間隔はG3電極23とG4電極2
4,G4電極24とG5電極25及びG5電極25と
G6電極26の各電極相互間隔を夫々b1b2b3とし、
対応する従来の電子銃電極構体1の電極間隔をa1
=a2=a3とすると、 b1=b2≧a,b1=b2>b3 の関係を満足するように設定されている。即ち陰
極線管製造工程中の高電圧処理時に接地電位され
るG3電極23、G5電極25に両側からはさまれ
る高電位電極となるG4電極24に対向する電極
間隔b1,b2を従来の対応する電極間隔と等しい
か、それ以上とし、接地電位にされるG5電極2
5と片側だけ対向する高電位電極となるG6電極
26との電極間隔b3を前記電極間隔b1,b2より小
さく設定する。但し電極相互間隔b1,b2は余り大
きいと外部電界の侵入の影響を受け、電子ビーム
通過孔中の電子ビーム径路を不所望に曲げてしま
うため、この影響を受けない大きさに選定し、b3
は余り小さいと電極相互間の耐電圧特性を劣化さ
せるため、これを劣化させることのない大きさに
選定されている。
First, the distance between the electrodes is G3 electrode 23 and G4 electrode 2.
4, G4 electrode 24, G5 electrode 25, and G5 electrode 25
The inter-electrode spacing of the G6 electrode 26 is respectively b 1 b 2 b 3 ,
The electrode spacing of the corresponding conventional electron gun electrode structure 1 is a 1
= a 2 = a 3 , the settings are made to satisfy the relationships b 1 = b 2 ≧a and b 1 = b 2 > b 3 . In other words, the electrode spacing b 1 and b 2 facing the G3 electrode 23, which is at ground potential during high voltage processing during the cathode ray tube manufacturing process, and the G4 electrode 24, which is a high potential electrode sandwiched from both sides by the G5 electrode 25, is changed from the conventional correspondence. G5 electrode 2, which is equal to or greater than the electrode spacing, and is at ground potential.
The electrode spacing b 3 between the G6 electrode 26 and the G6 electrode 26, which is a high potential electrode facing only one side, is set to be smaller than the electrode spacings b 1 and b 2 . However, if the inter-electrode spacings b 1 and b 2 are too large, they will be affected by the penetration of external electric fields and undesirably bend the electron beam path in the electron beam passage hole, so they should be selected to a size that will not be affected by this. , b 3
If it is too small, it will deteriorate the withstand voltage characteristics between the electrodes, so the size is selected so as not to cause this deterioration.

次にG3電極23〜G5電極25各組の閉塞筒状
体電極の軸方向長さは必要とする軸方向長さを二
等分割した長さでなく、異つた長さを持つた二つ
の閉塞筒状体電極23-1,23-2,24-1,24
-2,25-1,25-2の夫々が鍔状縁を重ね合せて
形成され、重ね合せられた鍔状縁の一部が絶縁物
支持杆19への支持子18となつている。各電極
の軸方向長さの分割は第4図に示す様に、G3電
極23とG4電極24、G4電極24とG5電極2
5、G5電極25とG6電極26の電極支持子18
間距離B1B2B3はその最小値を等分割した場合の
長さより大きくし、且つほぼ等しくなるように設
定されている。即ち電子ビーム進行方向である電
極軸方向長さが他の電極より小さく、電極間隔と
同等程度のG4電極24に対向するG3電極23、
G5電極25に於て、G3電極23のG4電極24に
対向するG3電極23-2の軸方向長さをG2電極1
2に対向するG3電極23-1より大きくなるよう
に分割し、G5電極25のG4電極24に対向する
G5電極25-1の軸方向長さをG5電極25-2より
大きくなるように分割し、電極支持子18間隔
B1B2を各電極の軸方向長を等分割したより大き
く設定し、G4電極24も可能な限り支持子間隔
B1B2が等しくなるように不等長をもつたG4電極
24-1,24-2に分割される。又G5電極25と
G6電極26の支持子間隔B3も他の間隔B1B2にほ
ぼ等しくなるようにG5電極25の軸方向分割比
は考慮される。
Next, the axial length of each set of closed cylindrical body electrodes from G3 electrode 23 to G5 electrode 25 is not the length obtained by dividing the required axial length into two, but two closed cylinders with different lengths. Cylindrical body electrodes 23 -1 , 23 -2 , 24 -1 , 24
-2 , 25 -1 , and 25 -2 are each formed by overlapping flanges, and a portion of the overlapping flanges serves as a support 18 for the insulator support rod 19. The axial length of each electrode is divided as shown in Figure 4: G3 electrode 23 and G4 electrode 24, G4 electrode 24 and G5 electrode 2.
5. Electrode supporter 18 for G5 electrode 25 and G6 electrode 26
The distance B 1 B 2 B 3 is set so that its minimum value is larger than the length when divided into equal parts, and is set to be approximately equal. That is, a G3 electrode 23 whose length in the electrode axial direction, which is the electron beam traveling direction, is smaller than other electrodes and which faces the G4 electrode 24, which is about the same as the electrode spacing;
In the G5 electrode 25, the axial length of the G3 electrode 23 -2 facing the G4 electrode 24 of the G3 electrode 23 is calculated as the G2 electrode 1
G3 electrode 23 facing 2 is divided so that it is larger than -1 , and facing G4 electrode 24 of G5 electrode 25
Divide the axial length of G5 electrode 25 -1 to be larger than G5 electrode 25 -2 , and divide the electrode supporter 18 intervals.
B 1 B 2 is set to be larger than the axial length of each electrode divided equally, and the G4 electrode 24 is also set with the support spacing as much as possible.
It is divided into G4 electrodes 24 -1 and 24 -2 having unequal lengths so that B 1 B 2 are equal. Also, with G5 electrode 25
The axial division ratio of the G5 electrode 25 is taken into consideration so that the support spacing B 3 of the G6 electrode 26 is also approximately equal to the other spacing B 1 B 2 .

上述した様に本発明の実施例によれば、主電子
レンズ構成電極の軸方向長さを異なる長さにした
ことと、及び電極の軸方向長さが対向電極間隙と
同程度、或いはそれ以下で高電圧が印加される
G4電極24に両側から対向するG3電極23、G5
電極25に対する電極間隔距離b1,b2を高電圧が
印加されるG6電極26に片側のみ対向するG5電
極25の両電極間隔距離b3より大きく設定した結
果各閉塞筒状体電極の軸方向長を等分割し、対向
電極相互間隔を等しくした場合より高電位差の生
じる各電極支持子間隔B1,B2,B3は可能の限り
大きく、且つ大略等しく設定されている。従がつ
て絶縁物支持杆19に沿つた電極支持子18間に
形成される最短漏洩電流径路も可能な限り大き
く、且つ大略等しくなり、陰極線管動作時に印加
される高電圧に対する耐電圧には十分の長さとな
り、又陰極線管製造工程中の高電圧処理工程では
印加高圧処理電圧を上昇させても最短漏洩電流径
路中の最小径路への漏洩電流の過大集中が防止出
来て、その処理電圧を大きく出来る。一方高電圧
処理時に接地電位されるG3電極23とG5電極2
5の二電極に両側からはさまれて高電位に保たれ
るG4電極24はその対向電極間隔b1,b2を接地
電位にされるG5電極25に片面だけ対向して高
電位に保たれるG6電極26との対向電極間隔b3
より大きく設定されているため、G3電極23と
G4電極24及びG4電極24とG5電極25間の電
界強度を、G5電極25とG6電極26間の電界強
度より弱く出来る。従がつて強電界による冷陰極
放出作用によるG4電極24からG3電極23、G5
電極25へ流入する冷陰極放出電流はG6電極2
6からG5電極25へ流入する電流より小さくな
る。即ちG3電極23、G5電極25から放出され
G4電極24表面に激突する電子の量及びその運
動エネルギーの夫々はG5電極25から放出され
G6電極26表面に激突する電子の量及び運動エ
ネルギーより小さくなるため、G4電極24の熱
容量がG6電極26と比べて著しく小さくても、
高電圧処理電圧を上昇させることにより、G4電
極24が異常に加熱され、赤熱することはなく、
電極支持子18の局部的熱で絶縁物支持杆19に
破壊に至る割れ目を生じることがなくなる。従が
つて高電位差の生じる電極支持子相互間隔を最大
限大きく、大略等しくすることと、電極相互間隔
を不等間隔とすることによる高電圧処理条件を全
ての電極間で一致出来るため、高電圧処理高圧を
高く出来て、電極間の耐電圧特性は著しく良好と
なる。
As described above, according to the embodiment of the present invention, the axial lengths of the electrodes constituting the main electron lens are set to different lengths, and the axial length of the electrodes is equal to or smaller than the gap between the opposing electrodes. high voltage is applied at
G3 electrode 23 and G5 facing G4 electrode 24 from both sides
As a result of setting the electrode spacing distances b 1 and b 2 with respect to the electrodes 25 to be larger than the electrode spacing distance b 3 of the G5 electrode 25, which faces only one side of the G6 electrode 26 to which a high voltage is applied, the axial direction of each closed cylindrical body electrode The electrode support spacings B 1 , B 2 , and B 3 , where a higher potential difference occurs than when the length is equally divided and the spacing between opposing electrodes is made equal, are set as large as possible and approximately equal. Therefore, the shortest leakage current path formed between the electrode supports 18 along the insulator support rods 19 is as large as possible and approximately equal, and is sufficient to withstand the high voltage applied during cathode ray tube operation. In addition, in the high-voltage processing process during the cathode ray tube manufacturing process, even if the applied high-voltage processing voltage is increased, excessive concentration of leakage current to the shortest path among the shortest leakage current paths can be prevented, and the processing voltage can be increased. It can be made big. On the other hand, G3 electrode 23 and G5 electrode 2 which are at ground potential during high voltage processing
The G4 electrode 24, which is held at a high potential by being sandwiched between two electrodes No. Opposite electrode spacing b 3 with G6 electrode 26
Since it is set larger, the G3 electrode 23 and
The electric field intensity between the G4 electrode 24 and the G4 electrode 24 and the G5 electrode 25 can be made weaker than the electric field intensity between the G5 electrode 25 and the G6 electrode 26. Therefore, G4 electrode 24 to G3 electrode 23, G5 due to the cold cathode emission effect due to a strong electric field.
The cold cathode emission current flowing into the electrode 25 is the G6 electrode 2.
6 to the G5 electrode 25. That is, it is released from the G3 electrode 23 and the G5 electrode 25.
The amount of electrons colliding with the surface of the G4 electrode 24 and their kinetic energy are both released from the G5 electrode 25.
Even if the heat capacity of the G4 electrode 24 is significantly smaller than that of the G6 electrode 26, it is smaller than the amount and kinetic energy of the electrons colliding with the surface of the G6 electrode 26.
By increasing the high voltage processing voltage, the G4 electrode 24 will not be abnormally heated and become red hot.
This eliminates the possibility of causing cracks in the insulator support rod 19 that could lead to destruction due to localized heat from the electrode supporter 18. Therefore, the high voltage processing conditions can be matched between all electrodes by making the mutual spacing between the electrode supports, which causes a high potential difference, as large as possible and making them approximately equal, and by making the mutual spacing between the electrodes unequal. The high processing pressure can be increased, and the withstand voltage characteristics between the electrodes are significantly improved.

以上の説明では主電子レンズ電極が4個からな
る電子銃電極構体について説明したが、4個以上
の電極構成であつて、高電圧の陽極電圧と中高電
圧の集束電圧が交互に周期的に印加される電子銃
電極構体に本願が適用出来ることはいうまでもな
い。
In the above explanation, an electron gun electrode structure consisting of four main electron lens electrodes has been described. However, in the case of an electrode structure with four or more electrodes, a high voltage anode voltage and a medium-high voltage focusing voltage are alternately and periodically applied. It goes without saying that the present application can be applied to an electron gun electrode structure.

又上述の説明では一体化電極を備えたインライ
ン型電子銃電極構体について説明したが、デルタ
型電子銃にも本願が適用出来ることもいうまでも
ない。
Further, in the above description, an in-line type electron gun electrode assembly including an integrated electrode has been described, but it goes without saying that the present invention can also be applied to a delta type electron gun.

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

第1図、第2図は従来の多段集束型電子レンズ
を備えたインライン型電子銃電極構体の夫々正面
図、側面図、第3図は第1図に示すA−A′断面
図、第4図は本発明の一実施例を示す多段集束型
電子レンズを備えたインライン型電子銃電極構体
の側面図を示す。 10……陰極構体、11……G1電極、12…
…G2電極、13-1,13-2,23-1,23-2……
G3電極、14-1,14-2,24-1,24-2……
G4電極、15-1,15-2,25-1,25-2……
G5電極、16,26……G6電極、18……電極
支持子、19……絶縁物支持杆。
1 and 2 are a front view and a side view, respectively, of an in-line electron gun electrode structure equipped with a conventional multi-stage focusing electron lens, and FIG. The figure shows a side view of an in-line electron gun electrode structure equipped with a multi-stage focusing electron lens, showing one embodiment of the present invention. 10... Cathode structure, 11... G1 electrode, 12...
...G2 electrode, 13 -1 , 13 -2 , 23 -1 , 23 -2 ...
G3 electrode, 14 -1 , 14 -2 , 24 -1 , 24 -2 ...
G4 electrode, 15 -1 , 15 -2 , 25 -1 , 25 -2 ...
G5 electrode, 16, 26...G6 electrode, 18...electrode supporter, 19...insulator support rod.

Claims (1)

【特許請求の範囲】[Claims] 1 陰極構体と、制御電極と、加速電極と、軸方
向の長さが異なる二つの閉塞筒状体電極をその電
極支持子用の鍔状縁で重ね合せて形成された第1
集束電極、第1陽極電極および第2集束電極と、
一個の閉塞筒状体電極よりなる第2陽極電極とが
それらの電極支持子を絶縁物支持杆に埋設するこ
とにより、この順序で配設されており、かつ第1
陽極電極とその両側の第1集束電極および第2集
束電極との相互の電極対向面間隔が共に第2集束
電極と第2陽極電極との相互の電極対向面間隔よ
り大きく設定され、さらに第1集束電極、第1陽
極電極、第2集束電極および第2陽極電極の電極
支持子相互間の最小の間隔が、軸方向の長さが等
しい二つの閉塞筒状体電極をその電極支持子用の
鍔状縁で重ね合せて第1集束電極、第1陽極電極
および第2集束電極を形成し、これらの電極対向
面間隔を等しくした場合の電極支持子相互間の最
小の間隔より大きく設定されていることを特徴と
する陰極線管電子銃電極構体。
1. A first electrode structure formed by overlapping a cathode structure, a control electrode, an acceleration electrode, and two closed cylindrical electrodes with different axial lengths at the flanged edge for the electrode supporter.
a focusing electrode, a first anode electrode, and a second focusing electrode;
A second anode consisting of one closed cylindrical electrode is arranged in this order by embedding their electrode supports in the insulator support rod, and the first
The mutual electrode facing distances between the anode electrode and the first focusing electrode and the second focusing electrode on both sides thereof are both set to be larger than the mutual electrode facing distances between the second focusing electrode and the second anode electrode, and The minimum distance between the electrode supports of the focusing electrode, the first anode electrode, the second focusing electrode, and the second anode electrode is such that the two closed cylindrical electrodes having the same axial length are used for their electrode supports. A first focusing electrode, a first anode electrode, and a second focusing electrode are formed by overlapping each other at the flanged edges, and the spacing between the opposing surfaces of these electrodes is set to be larger than the minimum spacing between the electrode supports. A cathode ray tube electron gun electrode structure characterized by:
JP41880A 1980-01-07 1980-01-07 Electron gun electrode frame for cathode-ray tube Granted JPS5697947A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP41880A JPS5697947A (en) 1980-01-07 1980-01-07 Electron gun electrode frame for cathode-ray tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP41880A JPS5697947A (en) 1980-01-07 1980-01-07 Electron gun electrode frame for cathode-ray tube

Publications (2)

Publication Number Publication Date
JPS5697947A JPS5697947A (en) 1981-08-07
JPH0146986B2 true JPH0146986B2 (en) 1989-10-12

Family

ID=11473245

Family Applications (1)

Application Number Title Priority Date Filing Date
JP41880A Granted JPS5697947A (en) 1980-01-07 1980-01-07 Electron gun electrode frame for cathode-ray tube

Country Status (1)

Country Link
JP (1) JPS5697947A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100778874B1 (en) * 2001-11-01 2007-11-22 엘지.필립스 디스플레이 주식회사 Electron gun for cathode ray tube

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5396756A (en) * 1977-02-04 1978-08-24 Matsushita Electronics Corp Picture tube unit
JPS54137959A (en) * 1978-04-19 1979-10-26 Toshiba Corp Structure and fabrication method of electron gun

Also Published As

Publication number Publication date
JPS5697947A (en) 1981-08-07

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