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JPH0744014B2 - Electron gun electrode - Google Patents
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JPH0744014B2 - Electron gun electrode - Google Patents

Electron gun electrode

Info

Publication number
JPH0744014B2
JPH0744014B2 JP61174473A JP17447386A JPH0744014B2 JP H0744014 B2 JPH0744014 B2 JP H0744014B2 JP 61174473 A JP61174473 A JP 61174473A JP 17447386 A JP17447386 A JP 17447386A JP H0744014 B2 JPH0744014 B2 JP H0744014B2
Authority
JP
Japan
Prior art keywords
points
opening
electron gun
electron
electrode
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP61174473A
Other languages
Japanese (ja)
Other versions
JPS6332838A (en
Inventor
一晃 内記
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
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP61174473A priority Critical patent/JPH0744014B2/en
Publication of JPS6332838A publication Critical patent/JPS6332838A/en
Publication of JPH0744014B2 publication Critical patent/JPH0744014B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、インライン型カラー陰極線管の電子銃電極に
関する。
TECHNICAL FIELD The present invention relates to an electron gun electrode for an in-line type color cathode ray tube.

〔従来の技術〕[Conventional technology]

陰極線管用電子銃の解像度は主として電子レンズの球面
収差に制約され、高解像度特性を得るためには主電子レ
ンズを構成する電極口径を大きくして、電子レンズの球
面収差を小さくする必要がある。電子ビームの通過する
3つの開口が一直線上に配列されたインライン型電子銃
では、単純に主電子レンズ口径を大きくすれば、開口間
距離である離心距離が大きくなるにしたがって、電子銃
を封止する陰極線管ネック径を大きくする必要がある。
The resolution of the electron gun for a cathode ray tube is limited mainly by the spherical aberration of the electron lens, and in order to obtain high resolution characteristics, it is necessary to increase the diameter of the electrode forming the main electron lens and reduce the spherical aberration of the electron lens. In an in-line type electron gun in which three apertures through which the electron beam passes are arranged in a straight line, if the diameter of the main electron lens is simply increased, the electron gun is sealed as the eccentric distance, which is the distance between the apertures, increases. It is necessary to increase the diameter of the neck of the cathode ray tube.

一般に、離心距離の増大は3本の電子ビームを蛍光面上
全域にわたって一点に集中させるコンバージェンス特性
を劣化させ、更にネック径の増大は陰極線管使用時に偏
向電力の増大を招き、いずれも望ましいことではない。
Generally, an increase in the eccentricity distance deteriorates the convergence property of concentrating three electron beams at one point on the entire fluorescent screen, and an increase in the neck diameter causes an increase in deflection power when a cathode ray tube is used. Absent.

そこで、インライン型電子銃の離心距離Sとネック径を
変更することなく、主電子レンズ構成電極の口径を大き
くする方法が従来提案されていた(特開昭60−9036)。
Therefore, there has been conventionally proposed a method of increasing the diameter of the electrode constituting the main electron lens without changing the eccentric distance S and the neck diameter of the in-line type electron gun (JP-A-60-9036).

第4図はこの従来例の要部切欠き斜視図、第5図はその
平面図、第6図は第5図A−Aの断面図、第7図は第4
図で示される電極を集束電極であるG3電極18と、陽極電
極であるG4電極19として互に対向させてバイ・ポテンシ
ャル・フォーカス方式主電子レンズを形成している電子
銃の側断面図である。
FIG. 4 is a perspective view of a notched part of this conventional example, FIG. 5 is its plan view, FIG. 6 is a sectional view of FIG. 5A-A, and FIG.
FIG. 3 is a side sectional view of an electron gun in which the electrodes shown in the drawing are opposed to each other as a focusing electrode G3 electrode 18 and an anode electrode G4 electrode 19 to form a bi-potential focus type main electron lens. .

この従来の電子銃電極は第4図に示されるように側面が
外部側壁13に覆われた筒状で、上面は第6図に示される
ように開口された主開口面3となっており、底面は最低
部が第1の閉塞面12となっており、第1の閉塞面12の長
手方向の中心線A−Aと、第1の閉塞面12のほぼ中心を
通り中心線A−Aと直行する第1の閉塞面12上の線Y−
Yと線Y−Yと距離Sだけ離れて線Y−Yに平行な平行
線X−X,Z−Zとが交わる3つの点a,b,cをそれぞれ中心
として中心点間距離Sより大きい直径DOで囲まれた部分
を所定高hOしぼり上げた形状とし、第1の閉塞面12と平
行な面を第2の閉塞面11としている。第1の閉塞面12と
第2の閉塞面11の間は三円重畳部側壁11WR,11WG,11WBで
接続されている。第1の閉塞面12で囲まれた三円重畳部
11WR,11WG,11WBはくびれ部17で仕切られた第1の開口面
11R,11G,11Bを有し、第1の開口面11R,11G,11Bから第2
の閉塞面11までを開口部R1,G1,B1としている。さら
に,第2の閉塞面11上の3点a,b,cを中心とし中心点間
距離Sより小さい直径D1でかこまれた3ヶ所を所定高h1
しぼり上げた形状とし内部筒状部16Wを残して3つの端
面を切除して3つの第2の開口面16R,16G,16Bが形成さ
れている。主開口面3の周囲には取付けと補強のための
電極支持子14、鍔状縁15が設けられている。
As shown in FIG. 4, this conventional electron gun electrode has a cylindrical shape whose side surface is covered by the outer side wall 13, and the upper surface is the main opening surface 3 which is opened as shown in FIG. The lowest part of the bottom surface is the first closed surface 12, and the center line A-A in the longitudinal direction of the first closed surface 12 and the center line A-A that passes through substantially the center of the first closed surface 12 A line Y- on the first obstruction surface 12 which goes orthogonally
It is larger than the distance S between the center points around the three points a, b, c where Y and the line Y-Y and the parallel lines X-X and Z-Z parallel to the line Y-Y are separated from each other by the distance S. A portion surrounded by the diameter D O has a shape of being squeezed up by a predetermined height h O , and a surface parallel to the first closing surface 12 is the second closing surface 11. The first closed surface 12 and the second closed surface 11 are connected by the side walls 11WR, 11WG, 11WB of the three-circle overlapping portion. Three-circle overlapping part surrounded by the first closing surface 12
11WR, 11WG, and 11WB are the first opening faces partitioned by the constricted part 17.
11R, 11G, 11B, from the first opening surface 11R, 11G, 11B to the second
Up to the closed surface 11 is defined as openings R 1 , G 1 , and B 1 . Furthermore, three points a, b, and c on the second closed surface 11 are centered, and three points surrounded by a diameter D 1 smaller than the distance S between the center points are predetermined heights h 1
Three second opening faces 16R, 16G, 16B are formed by cutting out three end faces while leaving the inner cylindrical portion 16W in a squeezed shape. An electrode support 14 and a brim 15 are provided around the main opening surface 3 for attachment and reinforcement.

この構造の電極を第7図に示すように、集束電極である
G3電極18と陽極電極であるG4電極19として対向させて形
成された電子レンズの球面収差は極めて小さく、中央及
び両外側電子レンズの開口配列方向である水平方向、こ
れに垂直な垂直方向のレンズ作用は等質となり、電子レ
ンズ内の占有電子ビーム径が大きくなる高電流域に至る
まで解像度特性は著しく向上する。
The electrode of this structure is a focusing electrode as shown in FIG.
The spherical aberration of the electron lens formed by facing the G3 electrode 18 and the G4 electrode 19 as the anode electrode is extremely small, and the lens in the horizontal direction, which is the aperture arrangement direction of the central and outer electron lenses, and the vertical direction perpendicular to this. The action is uniform, and the resolution characteristics are remarkably improved up to a high current region where the occupied electron beam diameter in the electron lens becomes large.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

上述した従来の電子銃電極は、第1の開口面11R,11G,11
B、開口部R1,G1,B1を形成する開口径D0を大きくし
て、開口部R1,G1,B1の相互の重畳度を大きくするに従
って、中央及び両外側電子レンズの球面収差は低減する
が、中央開口部G1と両外側開口部R1,B1間のくびれ部17
のくびれ量が少くなり、中央開口部G1の電子レンズでは
水平方向のレンズ作用が垂直方向より弱くなり、非点収
差が顕著となってくるため水平方向の最良フォーカス状
態を与える集束電圧が垂直方向の最良フォーカス状態を
与える集束電圧に対し低くなり、両者は一致しなくなっ
て、中央電子レンズで結像される蛍光面上の電子ビーム
スポットは著しく横長となり、従って、この型式の電子
レンズでは中央電子レンズによる解像度が両外側電子レ
ンズによる解像度より劣っている欠点がある。
The conventional electron gun electrode described above has the first opening surface 11R, 11G, 11
B, and increasing the opening R 1, G 1, B 1 opening diameter D 0 to form a according to increase the mutual superposition of the opening R 1, G 1, B 1, the central and two outer electron lens Spherical aberration is reduced, but the constriction 17 between the central opening G 1 and the outer openings R 1 and B 1 is 17
The constriction amount is small, and the lens action in the horizontal direction becomes weaker in the electron lens of the central aperture G 1 than in the vertical direction, and astigmatism becomes noticeable, so the focusing voltage that gives the best focus state in the horizontal direction is vertical. The focusing voltage that gives the best focus condition in the direction becomes low, and the two do not match, and the electron beam spot on the fluorescent screen imaged by the central electron lens becomes remarkably horizontal. Therefore, in this type of electron lens, The resolution of the electron lens is inferior to that of both outer electron lenses.

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

本発明の電子銃電極は、筒上であって上面は中心軸に直
角に交わる主開口面となっており、下面には主開口面と
平行な第1の閉塞面が形成され、第1の閉塞面上のその
ほぼ中心を通る直線上の等間隔の3点をそれぞれ中心と
する直径が前記間隔より大きい3つの円で囲まれた部分
を第1の開口面とするように所定高しぼり上げ、しぼり
上げた端面を第1の閉塞面と平行な第2の閉塞面とし、
第2の閉塞面上の前記3点のうち外側2点をそれぞれ中
心とする直径が前記間隔より小さい円と前記3点のうち
の真中の点を中心として前記3点を結ぶ直線方向を短径
とする前記外側2点を中心とする円とは交わらない楕円
とで囲まれた3個所を所定高しぼり上げそれぞれ筒状と
し、その端面をそれぞれ切除し第1の閉塞面と平行な3
つの開口面となる様に一体形成されている。
The electron gun electrode of the present invention has a cylindrical shape and an upper surface which is a main opening surface intersecting at right angles to the central axis, and a lower surface on which a first closed surface parallel to the main opening surface is formed. A predetermined height is raised so that a portion surrounded by three circles each having a diameter at each of three equally spaced points on a straight line passing through substantially the center of the closed surface as a center is larger than the spacing is the first opening surface. , The squeezed end surface is a second closing surface parallel to the first closing surface,
Of the three points on the second closed surface, a circle whose center is the outer two points is smaller than the interval and a straight line connecting the three points around the center point of the three points is a minor axis. The three points surrounded by an ellipse that does not intersect with the circle centered on the two outer points are squeezed by a predetermined height to form a cylindrical shape, and the end faces thereof are cut off to make the three parallel to the first closed surface.
They are integrally formed to form one opening surface.

したがって、本発明の電子銃電極を電子銃に適用すれ
ば、第1の開口部の中央部分で発生するレンズ作用の劣
化は、第2の閉塞面上に形成された楕円開口断面を有す
る筒状部分により補正される。
Therefore, when the electron gun electrode of the present invention is applied to an electron gun, the deterioration of the lens action occurring in the central portion of the first opening is caused by the cylindrical shape having the elliptical opening cross section formed on the second closed surface. It is corrected by the part.

〔実施例〕〔Example〕

次に、本発明の実施例について図面を参照して説明す
る。
Next, embodiments of the present invention will be described with reference to the drawings.

第1図は本発明の電子銃電極の一実施例を示す平面図、
第2図は第1図の要部切欠き斜視図、第3図は第1図の
A−A断面図である。従来例と同一記号をもつものは同
一部材を表わす。
FIG. 1 is a plan view showing an embodiment of an electron gun electrode of the present invention,
2 is a perspective view of a notched part of FIG. 1, and FIG. 3 is a sectional view taken along line AA of FIG. Those having the same symbols as in the conventional example represent the same members.

本実施例は、従来例における3つの中心点a,b,cが筒状
の電子銃電極の水平断面の中心線上に円形開口面16R,16
G,16Bを有する3つの内部筒状部分のうち、中央の開口
面16Gを有する部分を中心点bを通って中心線に直交す
る直線方向に長径D2を、中心線方向に短径を有する楕円
開口面26Gとする内部筒状部26Wを有している。ここで、
第1の閉塞面12の下面より第2の閉塞面11の下面までの
高さhOは中心点a,b,cを中心として第2の閉塞面をかこ
む円の直径DOの0.2〜0.6倍に設定されており、前記3つ
の内部筒状部分の高さは第2の閉塞面11の下面より同一
高h1に設定されている。
In this embodiment, the circular opening surfaces 16R, 16 are arranged on the center line of the horizontal section of the cylindrical electron gun electrode having the three central points a, b, c in the conventional example.
Of the three inner cylindrical portions having G and 16B, the portion having the central opening surface 16G passes through the center point b and has a major axis D 2 in a straight line direction orthogonal to the centerline and a minor axis in the centerline direction. It has an inner cylindrical portion 26W having an elliptical opening surface 26G. here,
The height h O from the lower surface of the first closed surface 12 to the lower surface of the second closed surface 11 is 0.2 to 0.6 of the diameter D O of the circle that encloses the second closed surface around the center points a, b, c. The height of the three inner cylindrical portions is set to be the same height h 1 from the lower surface of the second closing surface 11.

上記の電子銃電極2個を、例えば、第7図に示すと同様
に、集束電極18と陽極電極19として対向させてバイ・ポ
テンシャル・フォーカス型の電子レンズを構成するの
で、互に対向する第1の開口部R1,G1,B1に大口径で球
面収差の小さい電子レンズが形成される。然るに、開口
部R1,G1,B1の中央開口部G1と両外側開口部R1,B1間は
くびれ部17の部分で連通しているため、中央開口部G1
電子レンズは開口配列方向である水平方向のレンズ作用
が垂直方向より弱くなる非点収差が生じるが、内部筒状
部26Wの中央開口26Gは垂直方向に長軸を持った楕円形と
なっているため、第2の閉塞面11との接続部より第2の
開口面26Gに形成される電子レンズは逆に水平方向のレ
ンズ作用が垂直方向より強くなり、前記した中央開口部
G1のレンズ作用を相殺し、等質の非点収差のない電子レ
ンズとすることが出来る。一方、両外側開口部R1,B1
電子レンズは、中央開口部G1とはくびれ部17で連通して
いて、独立していないが、片側だけの連通のため中央開
口部G1程大きな非点収差は発生せず、その残留した非点
収差は第2の閉塞面11上に円筒形に形成された内部筒状
部16Wのレンズ作用で十分補償される。
As in the case of FIG. 7, the two electron gun electrodes are opposed to each other as the focusing electrode 18 and the anode electrode 19 to form a bi-potential focus type electron lens. An electron lens having a large diameter and a small spherical aberration is formed in each of the openings R 1 , G 1 , and B 1 of No. 1 . However, since the communication with the portion of the opening R 1, G 1, the central opening G 1 and both outer openings R 1 in B 1, B 1 between the constricted portion 17, central aperture electron lens in G 1 Causes astigmatism in which the lens action in the horizontal direction, which is the aperture arrangement direction, becomes weaker than in the vertical direction, but since the central aperture 26G of the internal tubular portion 26W is an elliptical shape having a long axis in the vertical direction, The electron lens formed on the second opening surface 26G from the connection portion with the second closing surface 11 has a stronger lens action in the horizontal direction than in the vertical direction.
By canceling the lens action of G 1 , it is possible to obtain a homogenous electron lens without astigmatism. On the other hand, the electron lenses of both outer openings R 1 and B 1 communicate with the central opening G 1 at the constricted portion 17 and are not independent, but because of communication on only one side, the central opening G 1 Large astigmatism does not occur, and the residual astigmatism is sufficiently compensated by the lens action of the inner cylindrical portion 16W formed in the cylindrical shape on the second blocking surface 11.

中央に形成される内部筒状部26Wの楕円状の第2の開口
面26Gの縦長度は第1の閉塞面12に形成された第1の開
口部R1,G1,B1の重畳度に従って決定すればよい。即
ち、第1の開口部R1,G1,B1径が大きくなって重畳度が
増加するに従って、第2の開口面26Gの楕円の長径を大
きくすればよい。楕円状の第2の開口面26Gの短径は必
ずしも上述したような両外側の第2の開口面16R,16Bの
開口径D1と一致させる必要はなく、中央及び両外側の電
子レンズの最適集束電圧が一致するように、その長径と
の兼ね合いで決定すればよい。
The longitudinal degree of the elliptical second opening surface 26G of the inner tubular portion 26W formed in the center is the superimposition degree of the first opening portions R 1 , G 1 , B 1 formed in the first closing surface 12. You can decide according to. That is, the major axis of the ellipse of the second opening surface 26G may be increased as the diameter of the first opening R 1 , G 1 , B 1 increases and the degree of superposition increases. The minor diameter of the elliptical second opening surface 26G does not necessarily have to match the opening diameter D 1 of the outer second opening surfaces 16R and 16B as described above, and is optimal for the central and outer electron lenses. It may be determined in consideration of the major axis so that the focusing voltages match.

上述の説明では主電子レンズがバイ・ポテンシャル・フ
ォーカス型をとる場合について説明したが、本発明はこ
れに限定されることなく、多段集束型電子レンズ等に適
用出来ることは云うまでもない。
In the above description, the case where the main electron lens is of the bi-potential focus type has been described, but it goes without saying that the present invention is not limited to this and can be applied to a multi-stage focusing electron lens or the like.

〔発明の効果〕〔The invention's effect〕

以上説明したように本発明は、3ヶ所に部分的に区切ら
れている第1の開口面から第2の閉塞面までの開口部の
中央部分は、両外側部分と異って、両外側部分に連結す
る方向のレンズ作用が弱いが、開口部の中央部分の直上
に楕円断面を有する内部筒状部分を設けることにより、
レンズ作用が補正され非点収差のない電子レンズを構成
する電子銃電極を実現できる効果がある。
As described above, according to the present invention, the central portion of the opening from the first opening surface to the second closing surface, which is partially divided into three parts, is different from both outer portions in both outer portions. Although the lens action in the direction of connecting to is weak, by providing an internal cylindrical portion having an elliptical cross section directly above the central portion of the opening,
There is an effect that it is possible to realize an electron gun electrode that constitutes an electron lens in which the lens action is corrected and has no astigmatism.

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

第1図は本発明の電子銃電極の一実施例を示す平面図、
第2図は第1図の要部切欠き斜視図、第3図は第1図A
−A断面図、第4,5,6図は従来例のそれぞれ要部切欠き
斜視図、平面図、A−A断面図、第7図は電子銃電極が
電子銃の中に組付けられているのを示す断面図である。 11……第2の閉塞面、12……第1の閉塞面、13……外部
側壁、14……電極支持子、15……鍔状縁、16R,26G,16B
……第2の開口面、16W,26W……内部筒状部、17……く
びれ部、11WR,11WG,11WB……三円重畳部側壁、11R,11G,
11B……第1の開口面、R1,G1,B1……第1の開口部。
FIG. 1 is a plan view showing an embodiment of an electron gun electrode of the present invention,
2 is a perspective view of a notched part of FIG. 1, and FIG. 3 is FIG. 1A.
-A sectional view, FIGS. 4, 5 and 6 are perspective views of a conventional example with a notched portion of each, a plan view, A-A sectional view, and FIG. 7 show an electron gun electrode assembled in an electron gun. FIG. 11 …… Second closing surface, 12 …… First closing surface, 13 …… External side wall, 14 …… Electrode supporter, 15 …… Brim edge, 16R, 26G, 16B
...... Second opening surface, 16W, 26W ...... Inner tubular part, 17 ...... Constricted part, 11WR, 11WG, 11WB ...... Side of three circle overlapping part, 11R, 11G,
11B: first opening surface, R 1 , G 1 , B 1 ... first opening portion.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】筒状の陰極線管用の電子銃電極であって、
上面は中心軸に直角に交わる主開口面となっており、下
面には主開口面と平行な第1の閉塞面が形成され、第1
の閉塞面上のそのほぼ中心を通る直線上の等間隔の3点
をそれぞれ中心とする直径が前記間隔より大きい3つの
円で囲まれた部分を第1の開口面とするように所定高し
ぼり上げ、しぼり上げた端面を第1の閉塞面と平行な第
2の閉塞面とし、第2の閉塞面上の前記3点のうち外側
2点をそれぞれ中心とする直径が前記間隔より小さい円
と前記3点のうちの真中の点を中心として前記3点を結
ぶ直線方向を短径とする前記外側2点を中心とする円と
は交わらない楕円とで囲まれた3個所を所定高しぼり上
げそれぞれ筒状とし、その端面をそれぞれ切除し第1の
閉塞面と平行な3つの第2の開口面となるように一体化
形成した電子銃電極。
1. An electron gun electrode for a cylindrical cathode ray tube, comprising:
The upper surface is a main opening surface intersecting at right angles to the central axis, and the lower surface has a first closed surface parallel to the main opening surface.
A predetermined height so that a portion surrounded by three circles having a diameter at each of three equally spaced points on a straight line passing through substantially the center of the closed surface of the above is larger than the spacing as the first opening surface A raised and squeezed end surface is used as a second closing surface parallel to the first closing surface, and a circle having a diameter centering on two outer points of the three points on the second closing surface is smaller than the interval. The three points surrounded by an ellipse that does not intersect with a circle centered on the outer two points having a minor axis in the direction of the straight line connecting the three points around the center of the three points are raised to a predetermined height. An electron gun electrode integrally formed into a cylindrical shape, each end surface of which is cut off to form three second opening surfaces parallel to the first closed surface.
JP61174473A 1986-07-23 1986-07-23 Electron gun electrode Expired - Lifetime JPH0744014B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61174473A JPH0744014B2 (en) 1986-07-23 1986-07-23 Electron gun electrode

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61174473A JPH0744014B2 (en) 1986-07-23 1986-07-23 Electron gun electrode

Publications (2)

Publication Number Publication Date
JPS6332838A JPS6332838A (en) 1988-02-12
JPH0744014B2 true JPH0744014B2 (en) 1995-05-15

Family

ID=15979094

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61174473A Expired - Lifetime JPH0744014B2 (en) 1986-07-23 1986-07-23 Electron gun electrode

Country Status (1)

Country Link
JP (1) JPH0744014B2 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0675378B2 (en) * 1989-11-08 1994-09-21 松下電子工業株式会社 Electron gun for color picture tube
US5731657A (en) 1992-04-21 1998-03-24 Hitachi, Ltd. Electron gun with cylindrical electrodes arrangement
US6411026B2 (en) 1993-04-21 2002-06-25 Hitachi, Ltd. Color cathode ray tube
JPH08190877A (en) 1995-01-09 1996-07-23 Hitachi Ltd Cathode-ray tube

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS609036A (en) * 1983-06-27 1985-01-18 Nec Corp Electron gun electrode assembly
JPS61131343A (en) * 1984-11-30 1986-06-19 Hitachi Ltd Electron gun for color picture tube

Also Published As

Publication number Publication date
JPS6332838A (en) 1988-02-12

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