JP2570700B2 - Electron gun electrode assembly - Google Patents
Electron gun electrode assemblyInfo
- Publication number
- JP2570700B2 JP2570700B2 JP61214431A JP21443186A JP2570700B2 JP 2570700 B2 JP2570700 B2 JP 2570700B2 JP 61214431 A JP61214431 A JP 61214431A JP 21443186 A JP21443186 A JP 21443186A JP 2570700 B2 JP2570700 B2 JP 2570700B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- diameter
- opening
- electron lens
- electron
- 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
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用電子銃の電
子レンズに於ける解像度を改善する電極構体に関するも
のである。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electrode assembly for improving the resolution of an electron lens of an in-line type color cathode ray tube electron gun.
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
る三つの開孔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、開孔
間距離である離心距離が大きくなると共に、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 an electron gun for a cathode ray tube is mainly limited by the spherical aberration of the electron lens. To obtain high resolution characteristics, it is necessary to increase the diameter of the electrode constituting 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 an electron beam passes are arranged in a straight line, simply increasing the aperture of the main electron lens increases the eccentric distance, which is the distance between the apertures, and seals the electron gun. It is necessary to increase the neck diameter of the cathode ray tube to be stopped.
一般に、離心距離の増大は三本の電子ビームを螢光面
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
偏向電力の増大をまねき、いずれも望ましいことではな
い。In general, an increase in the eccentric distance degrades the convergence characteristic of concentrating three electron beams at one point over the entire phosphor screen, and an increase in the neck diameter leads to an increase in the deflection power when a cathode ray tube is used. is not.
そこで第4図〜第6図に示す様に、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として、出願人
は特開昭60−9036号に示す様に三つの開孔離心距離S以
上の口径D0を持ち、三つの開孔を互いに重畳してインラ
イン配列した連通孔状の凹陥部を備え、その底部に突状
縁付独立開孔を備えた電極構造を提案している。Therefore, as shown in FIGS. 4 to 6, as a method of increasing the aperture of the main electron lens constituting electrode without changing the eccentric distance S and the neck diameter of the in-line type electron gun, the applicant has disclosed in Japanese Patent Application Laid-Open No. has a diameter D 0 of more than three apertures eccentricity distance S as shown in No. -9036, it includes a recessed portion of the communicating hole shape that is inline by superimposing the three apertures from each other, projecting with an edge at the bottom An electrode structure with independent openings is proposed.
第4図はこの提案に基づいた集束電極である閉塞筒状
体電極1の要部切欠き斜視図、第5図は上面図、第6図
は側断面図、第7図は上記構造の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
を形成した電子銃構体の側断面図を夫々示す。閉塞筒状
体電極1は第一閉塞面12に開孔離心距離S以上の口径D0
を持った三つの開孔11R,11G,11Bが互に重畳して欠円状
重畳形状となった連通孔凹陥部11が形成され、第一閉塞
面12に垂直な筒側部13の開放端側には閉塞面に平行な電
極支持子14を持った鍔状縁15が一体に形成されている。
凹陥部11は第一閉塞面12から開孔径D0の0.2〜0.6倍の距
離h0だけ離れた電極内部に形成され、その底面は第一閉
塞面12に平行な第二閉塞面を形成しており、三つの開孔
11R,11G11Bは互に連通され、重畳した三つの開孔周囲は
開孔重畳部にくびれ部17を持った連続した高さh0の側壁
11Wで囲まれている。FIG. 4 is a cutaway perspective view of a main part of the closed cylindrical body electrode 1 which is a focusing electrode based on this proposal, FIG. 5 is a top view, FIG. 6 is a side sectional view, and FIG. The focusing electrode is
Side sectional views of an electron gun structure in which a G3 electrode 18 and a G4 electrode 19 as an anode electrode are opposed to each other to form a bi-potential focus type main electron lens are shown. The closed cylindrical body electrode 1 has a diameter D 0 that is equal to or greater than the opening eccentric distance S on the first closed surface 12.
An opening end of a cylindrical side portion 13 perpendicular to the first closing surface 12 is formed with a communication hole recessed portion 11 in which three openings 11R, 11G, 11B having On the side, a flange-shaped edge 15 having an electrode support 14 parallel to the closing surface is integrally formed.
Recess 11 is formed in the internal electrode at a distance h 0 of 0.2 to 0.6 times the opening diameter D 0 from the first blocking surface 12, the bottom surface forms a second closing surface parallel to the first closing surface 12 Has three apertures
11R, 11G11B is mutually communicated, three apertures surrounding the superimposed continuous sidewall height h 0 with constricted portion 17 to the opening superimposing unit
Surrounded by 11W.
更に、連通孔状凹陥部の第二閉塞面11には三つの開孔
11R,11G,11Bと同軸でその開孔径D0より小さい口径D1を
持った、夫々が独立した完全円孔を形成した開孔16R,16
G,16Bが穿設され、その夫夫の口縁部は高さh1の突状縁1
6Wで囲まれている。Furthermore, three holes are formed in the second closed surface 11 of the communication hole-shaped concave portion.
11R, 11G, 11B coaxial its opening diameter with D 0 smaller diameter D 1, the opening to form a complete circular hole which respectively are independent 16R, 16
G, 16B is bored, protruding edges 1 of the rim height h 1 of the severally
Surrounded by 6W.
この構造の電極を第7図に示す様に、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
成された中央及び、両外側開孔部の電子レンズは重畳型
大口径部とこれに続く独立完全円孔部の相互作用で球面
収差は極めて小さく、中央及び両外側電子レンズの開孔
配列方向である水平方向、これに垂直な方向でのレンズ
作用は等質となり、電子レンズの解像度特性は著しく向
上する。The electrode having this structure is a focusing electrode as shown in FIG.
G 3 electrode 18 and the central and formed to face a G 4 electrode 19 is an anode electrode, an electron lens of a double outer apertures in the interaction of independent complete circular hole portion continuous thereto and the superposition type large diameter portion The spherical aberration is extremely small, and the lens action in the horizontal direction, which is the direction in which the apertures of the central and outer electron lenses are arranged, and in the direction perpendicular thereto is uniform, and the resolution characteristics of the electronic lens are significantly improved.
然るに、上記構造の電極構造では三つの開孔が互に重
畳されてインライン配列された連通孔状の凹陥部底面に
突状縁付の独立した完全円孔が一体形成されているため
構造が比較的複雑となり電極形成加工が困難となる欠点
があった。この場合、連通孔状凹陥部の形成、及び凹陥
部底面内に所定高さh1を持った突状縁付独立円孔の形成
が特に困難となる。However, in the electrode structure of the above structure, the three holes are superimposed on each other, and an independent perfect circular hole with a protruding edge is integrally formed on the bottom surface of the communicating hole-shaped concave portion which is arranged inline. However, there is a disadvantage that the electrode formation processing becomes difficult and the electrode forming process becomes difficult. In this case, the formation of the communication hole shaped recess, and the formation of the projecting edge with separate circular hole having a predetermined height h 1 in the recess in the bottom surface is particularly difficult.
更に、第一閉塞面12の重畳形開孔径D0を大きくして、
その開孔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一層低減するが、中央開
孔11Gと両外側開孔11R,11B間のくびれ部17の幅が大きく
なり、中央開孔部の電子レンズは水平方向の集束作用が
垂直方向より弱くなる非点収差が顕著となってくる。こ
のため水平方向の最適集束電圧が垂直方向のそれより低
くなり、中央電子レンズで結像される螢光面上の電子ビ
ームスポットは著しく横長となり、その解像度は両外側
電子レンズより劣化する欠点があった。Furthermore, by increasing the superposition type opening diameter D 0 of the first closing surface 12,
As the degree of superposition of the apertures is increased, the spherical aberration of the central and both outer electron lenses is further reduced, but the width of the constricted portion 17 between the central aperture 11G and both outer apertures 11R and 11B increases, The astigmatism in which the focusing action in the horizontal direction is weaker than that in the vertical direction becomes remarkable in the electron lens in the central aperture. Therefore, the optimal focusing voltage in the horizontal direction is lower than that in the vertical direction, the electron beam spot on the phosphor screen formed by the central electron lens becomes extremely long, and its resolution is deteriorated compared to the outer electron lenses. there were.
本発明は上述の欠点に鑑みてなされたものであり、閉
塞面に三つの開孔を互に重畳させてインライン配列した
連通孔状開孔を穿設した電極と、この電極内部に突状縁
付独立開孔を備え、前記閉塞面から所定距離隔てて対向
させた電極を配設した電極構体によって主電子レンズを
構成し、電極形成加工上の困難や、寸法上の制約に限定
されることなく、且、中央及び両外側電子レンズの解像
度特性を均一にし、解像度の極めて優ぐれ、単純な構成
で、その電極形成が容易な電極を有した電子銃電極構体
を提供するものである。The present invention has been made in view of the above-described drawbacks, and has an electrode in which three closed holes are overlapped with each other on a closed surface to form a communication hole formed in-line and a protruding edge is formed inside the electrode. The main electron lens is constituted by an electrode assembly having an independent opening and an electrode disposed at a predetermined distance from the closed surface to face the main electron lens, and is limited to difficulties in electrode formation processing and dimensional restrictions. An object of the present invention is to provide an electron gun electrode assembly having electrodes having a uniform structure, uniform resolution characteristics of the center and both outer electron lenses, an extremely excellent resolution, a simple structure, and electrodes which can be easily formed.
本発明は、閉塞筒状体電極の閉塞面にインライン配列
される三つの開孔間離心距離以上の開孔径を持ち、三つ
の開孔を互に重畳させて円弧のみで構成された連通孔を
その孔部が閉塞面から突出することなく穿設し、この電
極内部に突状縁付独立開孔を備えて、前記閉塞面から所
定距離隔てられ、且つ突状縁先端が閉塞面と反対側に突
出するように設置される入れ子状の補助電極とで主電子
レンズ電極を構成し、一対の前記電極構体を連通孔穿設
面が互に対向するように離間させて主電子レンズを形成
し、相対的に高電位にある電極構体の連通孔径を低電位
側のそれより相対的に小さく設定すると共に、上記電極
構体の少くとも一方の連通孔の中央開孔径を両外側より
小さくしたものである。The present invention has a hole diameter of not less than the eccentric distance between the three holes arranged in-line on the closed surface of the closed cylindrical electrode, a communication hole formed only by an arc by overlapping the three holes mutually. The hole is bored without protruding from the closed surface, and an independent opening with a protruding edge is provided inside the electrode, a predetermined distance from the closed surface, and the tip of the protruding edge is on the opposite side to the closed surface. A main electron lens electrode is constituted by a nested auxiliary electrode installed so as to protrude into the main electron lens, and the main electron lens is formed by separating the pair of electrode assemblies so that the communication hole perforated surfaces face each other. In addition, the diameter of the communication hole of the electrode structure at a relatively high potential is set relatively smaller than that of the electrode structure on the low potential side, and the center opening diameter of at least one of the communication holes of the electrode structure is smaller than that on both outer sides. is there.
この様に電極を構成することによって、主電子レンズ
部を構成する開孔部構造を非常に単純化出来、その電極
成形は容易となり、更に重畳形開孔径は従来の凹陥部を
有した電極より一層大きく設定することが可能となり、
中央と両外側開孔部の電子レンズ作用を開孔配列方向で
ある水平、及びこれと垂直方向とで同一にして解像度特
性の極めて優ぐれた大口径電子レンズとすることが可能
となる。By configuring the electrodes in this manner, the aperture structure of the main electron lens can be greatly simplified, the electrode can be easily formed, and the overlapped aperture diameter is larger than that of a conventional electrode having a concave portion. It is possible to set it even larger,
By making the electron lens action of the center and the outer opening portions the same in the horizontal and vertical directions in which the apertures are arranged, a large-diameter electron lens with extremely excellent resolution characteristics can be obtained.
以下に図面を参照して本発明の実施例を詳細に説明す
る。Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.
第1図は本発明の一実施例に基づく電極構体をG3電極
2、G4電極4として対向配置してバイ・ポテンシャル・
フォーカス型電子レンズを構成した電子銃電極構体の要
部側断面図を、第2図(a),(c)は前記G3電極2を
構成する閉塞筒状体電極20の斜視図、上面図、及び
(b)は前記電極20へ入子状に配設される補助電極3の
斜視図を、第3図はG4電極4を構成する閉塞筒状体電極
40の上面図を示す。FIG. 1 shows an electrode structure according to an embodiment of the present invention as a G3 electrode 2 and a G4 electrode 4 which are opposed to each other.
2 (a) and 2 (c) are a perspective view, a top view, and a sectional view, respectively, showing a closed cylindrical body electrode 20 constituting the G3 electrode 2. FIG. 3 (b) is a perspective view of an auxiliary electrode 3 nested on the electrode 20, and FIG. 3 is a closed cylindrical electrode constituting a G4 electrode 4.
40 shows a top view.
閉塞筒状体電極20は第2図(a)に示す様に、大略長
円形状の閉塞面22とこれに垂直な筒側部23及びこれに連
続して筒側部23に垂直に張り出された電極支持子24を持
った鍔状縁25が一体に形成されている閉塞面22には開孔
間中心距離である開孔離心距離S以上の開孔径DAを持っ
てインライン配列された中央及び両外側開孔21G,21R,21
Bを重畳させて円の一部を欠き、円弧のみで構成された
欠円状重畳型形状となった連通孔21が穿設されている。As shown in FIG. 2 (a), the closed tubular body electrode 20 extends substantially perpendicularly to the closed side 22 having a substantially elliptical shape, a cylindrical side portion 23 perpendicular thereto, and the cylindrical side portion 23 continuously therefrom. flange-like rim 25 having an electrode Shijiko 24 which are are line arrangement with an aperture eccentricity distance S above opening diameter D a is the opening between the center distance is the closing surface 22 formed integrally Center and both outer holes 21G, 21R, 21
A communication hole 21 is formed in which a part of a circle is missing by superimposing B, and a communication hole 21 having a partially circular superimposed shape constituted only by an arc is formed.
第2図(b)に示す補助電極3は第1図中に示す様
に、G3電極2、G4電極4を構成する閉塞筒状体電極20,4
0の内側に入子状に嵌合する同じく閉塞筒状体であり、
閉塞面32とこれに垂直な筒側部33、筒側部に垂直に張り
出された前述の鍔状縁25に一致する電極支持子34を持っ
た鍔状縁35が一体に形成されている。閉塞面32には開孔
離心距離S以下で完全円孔を形成する口径D1を持ってイ
ンライン配列された三つの開孔31R,31G,31Bが穿設さ
れ、その夫々は内部に突出し、高さh1の突状縁31Wで囲
まれている。閉塞筒状体電極20と補助電極3の筒側部長
は第1図に示す様に、補助電極3を閉塞筒状体電極20内
に嵌合させて鍔状縁25,35を重ね合せた時、双方の閉塞
面間距離が所定の高さh0となるように設定されている。As shown in FIG. 1, the auxiliary electrodes 3 shown in FIG. 2 (b) are closed cylindrical electrodes 20, 4 constituting the G3 electrode 2 and the G4 electrode 4.
It is also a closed cylindrical body that fits telescopically inside 0,
A closed surface 32, a cylindrical side portion 33 perpendicular to the closed surface 32, and a flanged edge 35 having an electrode support 34 corresponding to the aforementioned flanged edge 25 projecting vertically to the cylindrical side portion are integrally formed. . Inline arranged with a diameter D 1 to form a completely circular hole in the following opening eccentricity distance S is in the closed surface 32 a three apertures 31R, 31G, 31B is bored, its respective protrudes inside, high It is surrounded by a protruding edge 31W of h 1. As shown in FIG. 1, the cylinder side length of the closed cylindrical body electrode 20 and the auxiliary electrode 3 is determined when the auxiliary electrode 3 is fitted into the closed cylindrical body electrode 20 and the flanges 25 and 35 are overlapped. , the distance between both closing surface is set to a predetermined height h 0.
一方、G4電極4を構成する閉塞筒状体電極40は第3図
に示す様に閉塞筒状体電極20と大略同一形状の閉塞筒状
体であって、長円形状の閉塞面42とこれに垂直な筒側部
43、これに垂直に張出された電極支持子44を持った鍔状
縁45が一体に形成されている。閉塞面42には前述のG3電
極2の開孔離心距離Sより若干大きいS′以上の中央開
口径DC、両外側開口径DSを持ってインライン配列された
中央及び両外側開孔41G,41R,41Bを重畳させて円弧のみ
で構成された欠円状重畳型形状となった連通孔41が穿設
されている。On the other hand, as shown in FIG. 3, the closed cylindrical body electrode 40 constituting the G4 electrode 4 is a closed cylindrical body having substantially the same shape as the closed cylindrical body electrode 20, and includes an oval closed surface 42 and an oval closed surface 42. Tube side perpendicular to
43, a flange-like edge 45 having an electrode support 44 extending perpendicularly thereto is integrally formed. The closing surface 42 is slightly larger than the opening eccentricity distance S above the G3 electrode 2 S 'or more central opening diameter D C, is line arrangement with both outer opening diameter D S central and two outer apertures 41G, A communication hole 41 is formed by superimposing 41R and 41B to form a partially circular superimposed type formed only by an arc.
然るに、G3電極2とG4電極4の開孔径と離心距離の関
係は、DA>DS>DC>S′≧Sとなっており、G4電極4の
開孔径DS,DCはいずれも相対的にG3電極の開孔径DAより
小さく、且つその連通孔の中央開孔41Gは両外側開孔41
R,41Bより小さく設定されている。However, the relationship between the opening diameters of the G3 electrode 2 and the G4 electrode 4 and the eccentric distance is D A > D S > D C > S ′ ≧ S, and the opening diameters D S and D C of the G 4 electrode 4 are either smaller than the opening diameter D a relatively G3 electrode also and central aperture 41G is two outer apertures of the communicating hole 41
It is set smaller than R and 41B.
第1図に示す様に、閉塞筒状体電極20に補助電極3を
嵌合させG3電極とし、同じく閉塞筒状体電極40に補助電
極3′(補助電極3の離心距離Sに対しS′としたも
の)を嵌合させてG4電極4とし、所定距離隔て連通孔部
を対向させてバイ・ポテンシャル・フォーカス型の電子
レンジを形成すれば、重畳型大口径を持った連通孔21,4
1と、その奥の突状縁を持った独立開孔部31R,31R′;31
G,31G′;31B,31B′の夫々とで電子レンズが形成され
る。重畳型大口径電子レンズと独立の小口型電子レンズ
の合成効果としてG3電極2とG4電極4の対向部には独立
した球面収差の極めて小さい大口径電子レンズが形成さ
れたことになる。As shown in FIG. 1, the auxiliary electrode 3 is fitted to the closed cylindrical body electrode 20 to form a G3 electrode, and the closed cylindrical body electrode 40 is similarly connected to the auxiliary electrode 3 '(S' with respect to the eccentric distance S of the auxiliary electrode 3). The G4 electrodes 4 are fitted together to form a bi-potential focus type microwave oven with the communication holes facing each other at a predetermined distance to form the communication holes 21 and 4 having a superposed large diameter.
1 and independent opening portions 31R, 31R '; 31 with protruding edges at the back
G, 31G '; 31B, 31B' form an electron lens. As a combined effect of the superposition type large-aperture electron lens and the independent small-aperture electron lens, an independent large-aperture electron lens having extremely small spherical aberration is formed at the opposing portion of the G3 electrode 2 and the G4 electrode 4.
一方、第1図に示すG3電極2側の独立開孔31R,31G,31
Bが形成された閉塞面32と連通孔21が形成された閉塞面2
2間の距離h0は計算機を用いたシュミレーションと実験
により、重畳型開孔径DA,DSの0.2〜0.6倍程度に選べば
最良の集束特性が得られることを用いだした。On the other hand, the independent openings 31R, 31G, 31 on the G3 electrode 2 side shown in FIG.
Closed surface 32 with B formed and closed surface 2 with communication hole 21 formed
The distance h 0 between 2 and simulation using the computer simulation, the superposition type opening diameter D A, began with the best focusing properties are obtained if you choose to 0.2 to 0.6 times the D S.
この関係はG4電極4側でも同様に成立する。 This relationship is similarly established on the G4 electrode 4 side.
一般に、バイ・ポテンシャル・フォーカス型電子レン
ズでは集束電圧が印加されるG3電極2側には集束レンズ
が形成され、陽極電圧が印加されるG4電極4側に発散レ
ンズが形成される。又、重畳型開孔電子レンズではイン
ライン開孔配列方向と垂直方向開孔径が水平方向開孔径
より小さくなるため、垂直方向の集束作用は水平方向よ
り強くなり、螢光面上の電子ビームスポットは横長に歪
む。特に中央開孔は両外側部に仕切りがなくなるため、
中央電子レンズでは両外側電子レンズより垂直方向集束
作用が水平方向集束作用より著しく強くなり、最適集束
電圧が垂直方向と水平方向で大きく異る非点収差が顕著
となる。In general, in a bi-potential focus type electron lens, a focusing lens is formed on the G3 electrode 2 side to which a focusing voltage is applied, and a diverging lens is formed on the G4 electrode 4 side to which an anode voltage is applied. Also, in the superimposed apertured electron lens, the aperture diameter in the in-line aperture arrangement direction and the aperture diameter in the vertical direction are smaller than the aperture diameter in the horizontal direction, so that the focusing action in the vertical direction is stronger than in the horizontal direction, and the electron beam spot on the fluorescent surface is Distorted horizontally. Especially since the central opening has no partitions on both outer parts,
In the central electron lens, the focusing effect in the vertical direction is significantly stronger than the focusing effect in the horizontal direction as compared with the outer electron lenses, and astigmatism in which the optimum focusing voltage greatly differs between the vertical direction and the horizontal direction becomes remarkable.
然るに、本願ではG4電極4の重畳型開孔41の開孔径は
G3電極2のそれより小さく設定されているため、G4電極
4側に形成される発散レンズは両者を同径とした場合よ
り強くなる。逆に集束レンズ作用は弱くなり、特に垂直
方向の集束作用がG3電極2側と同径の場合より弱くな
り、水平、垂直方向の最適集束電圧を一致させることが
出来る。However, in the present application, the opening diameter of the overlap type opening 41 of the G4 electrode 4 is
Since it is set to be smaller than that of the G3 electrode 2, the diverging lens formed on the G4 electrode 4 side is stronger than when both have the same diameter. Conversely, the function of the focusing lens is weakened, and in particular, the focusing action in the vertical direction is weaker than when the diameter is the same as that of the G3 electrode 2, so that the optimum focusing voltages in the horizontal and vertical directions can be matched.
更に、G4電極4側の連通孔41の中央開孔41Gの口径DC
は両外側開孔41R,41Bの口径DSより小さく設定されてい
るため、中央開孔41Gの垂直方向集束作用を中央及び両
外側開孔共等径とした場合より弱めることが可能となっ
た。従って、口径DCを適切に選ぶことによって、中央開
孔41Gの垂直方向集束作用を弱めて、水平、垂直方向最
適集束電圧を一致させることが出来て、中央及び両外側
開孔部の電子レンズ集束作用を均一にし、電子ビームス
ポットの横長歪を補正して円形状とし、その非点収差を
除去出来る。Further, the diameter D C of the central opening 41G of the communication hole 41 on the G4 electrode 4 side.
Is set smaller than the diameter D S of both outer openings 41R and 41B, so that the vertical focusing action of the central opening 41G can be weakened compared to the case where both the center and both outer openings have the same diameter. . Therefore, by choosing the diameter D C appropriately, weakening the vertical focusing action of the central aperture 41G, horizontal, to be able to match the vertical optimum focusing voltage, the central and two outer apertures electron lens The focusing action is made uniform, the horizontal distortion of the electron beam spot is corrected to form a circular shape, and the astigmatism can be removed.
また、くびれ部47の幅Gは三つの連通孔部口径を等し
くした場合より小さく出来るため、両外側開孔部電子レ
ンズの中央開孔側レンズ集束作用を強めることが可能と
なり、その水平、垂直方向のレンズ作用を均一に出来
て、解像度の極めて優れた電子レンズとすることが出来
る。Also, since the width G of the constricted portion 47 can be made smaller than when the diameters of the three communication holes are equal, it is possible to enhance the central aperture side lens converging action of the both outer aperture electron lenses, and to increase the horizontal and vertical The lens function in the directions can be made uniform, and an electronic lens with extremely excellent resolution can be obtained.
この様な電極構成にすることで、開孔離心距離S以上
の大口径を持った連通孔部21,41は閉塞面22,42へ単に連
通孔状開孔を穿設するだけでよく、その周囲に側壁を形
成する必要がないため、その孔部形成は極めて容易とな
り、部品加工の量産性が非常に高い。また、その連通孔
21,41周囲には側壁が不要であるため、開孔径は電極形
成に伴う寸法上の制約を考慮する必要がなく、閉塞面2
2,42の短辺幅以下なら任意に大きく設定可能となる。一
方、補助電極3は連通孔部を持った電極本体と別に形成
されるため、両者の相対距離h0、突状縁の高さh1やその
開孔径D1は連通孔の形状に一切制限されることなく自由
に設定可能であり、やはりその電極形成は極めて容易と
なる。With such an electrode configuration, the communication holes 21 and 41 having a large diameter larger than the opening eccentric distance S may be formed by simply forming communication holes in the closed surfaces 22 and 42. Since there is no need to form a side wall around the periphery, the formation of the hole becomes extremely easy, and the mass productivity of component processing is extremely high. Also, its communication hole
No side wall is required around 21,41, so it is not necessary to consider the dimensional restrictions associated with electrode formation.
If it is less than the short side width of 2,42, it can be set arbitrarily large. On the other hand, since the auxiliary electrode 3 is formed separately from the electrode main body having the communication hole, the relative distance h 0 , the height h 1 of the protruding edge, and the opening diameter D 1 thereof are all limited to the shape of the communication hole. It can be set freely without being performed, and the electrode formation is also extremely easy.
以上の説明でG3電極2の開孔離心距離Sに対し、G4電
極4のそれをSより若干大きいS′としたが、これはよ
く知られている様に三つの陰極からG3電極2内迄は電子
銃の軸20R,20G,20B上を平行に進んで来た三本の電子ビ
ームを螢光面上で静電気的に一点に集中させるため、G4
電極4の連通孔41か、補助電極3′の独立開孔の少くと
もいずれか一方の外側開孔中心を外側に偏心させるため
である。In the above description, the opening eccentric distance S of the G3 electrode 2 is set to S 'which is slightly larger than S of the G4 electrode 4. As is well known, this is from the three cathodes to the inside of the G3 electrode 2. G3 is used to electrostatically concentrate the three electron beams that have traveled in parallel on the axes 20R, 20G, and 20B of the electron gun on the fluorescent screen at one point.
This is because the center of at least one of the communication hole 41 of the electrode 4 and the independent opening of the auxiliary electrode 3 'is decentered outward.
更に、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行ったが、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
等にも適用出来ることは云うまでもない。Further, in the above description, the case where the main electron lens is of a bi-potential focus type has been described. However, the present invention is not limited to this, and it is needless to say that the present invention can be applied to a multi-stage focusing type electron lens and the like. Absent.
以上述べた様に、開孔離心距離以上の大口径を持った
連通孔部は閉塞筒状体電極の閉塞面に重畳型欠円状の連
通孔を穿設するだけでよく、開孔部形成は非常に容易
で、且つその孔径は閉塞面の短辺幅以下なら任意に大き
く設定出来て、簡単な構成により中央及び両外側電子レ
ンズの水平、垂直方向集束特性を一致させて、大口径電
子レンズ部による解像度特性を著しく向上させることが
出来る。その上、連通孔状大口径電子レンズ部に対向す
る突状縁付開孔を備えた補助電極は連通孔部をもった電
極本体と別になっていて、入れ子状に嵌合させるだけで
よいため、両者の相対位置や、突状縁の径や高さを前者
の連通孔形成との関係で制約される寸法上の制限を一切
受けないで任意に設定可能であり、独立開孔部を構成す
る補助電極形成が容易であるばかりでなく、電子レンズ
系の最適設計が容易となる。As described above, the communication hole portion having a large diameter larger than the opening eccentric distance only needs to form a superimposition-shaped oval communication hole on the closed surface of the closed cylindrical electrode, and the opening portion is formed. Is very easy, and the hole diameter can be set arbitrarily large as long as it is less than the short side width of the closed surface, and the horizontal and vertical focusing characteristics of the center and both outer electron lenses can be matched by a simple configuration, The resolution characteristics of the lens unit can be significantly improved. In addition, since the auxiliary electrode having a protruding edged opening facing the communication hole-shaped large-diameter electron lens portion is separate from the electrode body having the communication hole portion, it is only necessary to fit in a nested manner. , The relative position of the two, and the diameter and height of the protruding edge can be set arbitrarily without any dimensional restrictions constrained by the relationship with the formation of the communication hole, and constitutes an independent aperture Not only is it easy to form auxiliary electrodes, but also the optimal design of the electron lens system is facilitated.
第1図は本発明の一実施例に基づく電極構体をG3電極、
G4電極として対向配置してバイ・ポテンシャル・フォー
カス型電子レンズを構成した電子銃電極構体の要部側断
面図を、第2図(a),(b)は前記G3電極を構成する
閉塞筒状体電極の斜視図、及び(c)は前記電極内へ入
子状に配設される補助電極の斜視図を、第3図はG4電極
を構成する閉塞筒状体電極の上面図を、第4図は本発明
に先駆けて提案された閉塞筒状体電極の要部切欠き斜視
図、第5図、第6図はそれの上面図、側断面図、第7図
は前記構造の電極を集束電極であるG3電極と、陽極電極
であるG4電極として対向配置してバイ・ポテンシャル・
フォーカス型電子レンズを構成した電子銃電極構体の側
断面図を夫々示す。 1,20,30……閉塞筒状体電極、3,3′……補助電極、11…
…凹陥部(第二閉塞面)、12……第一閉塞面、22,32,42
……閉塞面、13,23,33,43……筒側部、14,24,34,44……
電極支持子、15,25,35,45……鍔状縁、11R,11G,11B;21
R,21G,21B;41R,41G,41B……欠円状重畳型開孔、21,41…
…連通孔、17,27,47……くびれ部、16R,16G,16B;31R,31
G,31B……完全円孔状開孔、16W,31W……突状縁、11W…
…凹陥部側壁、20R,20G,20B……電子銃の軸、DC……欠
円状重畳型開孔の中央開孔径、DS……欠円状重畳開孔の
両外側開孔径。FIG. 1 shows an electrode assembly according to one embodiment of the present invention as a G3 electrode,
FIGS. 2 (a) and 2 (b) are cross-sectional views of a main part of an electron gun electrode structure in which a bi-potential focus type electron lens is arranged facing each other as a G4 electrode. FIG. 3C is a perspective view of a body electrode, FIG. 3C is a perspective view of an auxiliary electrode nested in the electrode, FIG. 3 is a top view of a closed cylindrical body electrode constituting a G4 electrode, FIG. FIG. 4 is a cutaway perspective view of a main part of the closed tubular body electrode proposed prior to the present invention, FIGS. 5 and 6 are top views, side sectional views, and FIG. G3 electrode as a focusing electrode and G4 electrode as an anode electrode
The side sectional views of the electron gun electrode structure constituting the focus type electron lens are respectively shown. 1,20,30 …… Closed cylindrical electrode, 3,3 ′ …… Auxiliary electrode, 11…
... recessed part (second closed surface), 12 ... first closed surface, 22, 32, 42
…… Closed surface, 13,23,33,43 …… Cylinder side, 14,24,34,44 ……
Electrode support, 15,25,35,45 ......... Flanged edge, 11R, 11G, 11B; 21
R, 21G, 21B; 41R, 41G, 41B …… Circular overlapping superimposed holes, 21,41…
… Communication holes, 17, 27, 47 …… Constrictions, 16R, 16G, 16B; 31R, 31
G, 31B …… Full circular opening, 16W, 31W …… Projecting edge, 11W…
... recess sidewall, 20R, 20G, 20B ...... electron gun axis, D C ...... segmental shaped superposition type opening of the central opening diameter, both outer opening diameter of D S ...... segmental shape superimposed aperture.
Claims (1)
される三つの開孔間離心距離以上の開孔径を持ち、三つ
の開孔を互いに重畳させて、円弧のみで構成された連通
孔をその孔部が閉塞面から突出することなく穿設し、こ
の電極内部に突状縁付独立開孔を備えて、前記閉塞面か
ら所定距離隔てられ、且つ突状縁先端が閉塞面と反対側
に突出するように設置される入れ子状の補助電極とで主
電子レンズ電極構体を構成し、一対の前記電極構体を連
通孔穿設面が互いに対向するように離間させて主電子レ
ンズを形成して、相対的に高電位側にある電極構体の連
通孔の各々の径を低電位側の連通孔の各々の径より相対
的に小さく設定すると共に、前記電極構体の少なくとも
一方の連通孔中央開孔径を両外側開孔径より小さくした
ことを特徴とする電子銃電極構体。A communication hole having an opening diameter greater than the eccentric distance between three openings arranged in-line on the closing surface of the closing cylindrical electrode, and having three openings overlapping each other to form only a circular arc. A hole is formed without protruding from the closed surface, an independent opening with a protruding edge is provided inside the electrode, a predetermined distance is provided from the closed surface, and the protruding edge tip is opposite to the closed surface. A main electron lens electrode structure is constituted by a nested auxiliary electrode installed so as to protrude to the side, and the main electron lens is formed by separating a pair of the electrode structures so that the communication hole perforated surfaces face each other. The diameter of each of the communication holes of the electrode assembly on the relatively high potential side is set relatively smaller than the diameter of each of the communication holes on the low potential side, and the center of at least one of the communication holes of the electrode assembly is set. The opening diameter is smaller than the opening diameter on both sides. Child gun electrode structure.
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61214431A JP2570700B2 (en) | 1986-09-10 | 1986-09-10 | Electron gun electrode assembly |
KR1019870001152A KR910001157B1 (en) | 1986-02-12 | 1987-02-12 | Electrode assembly for electrostatic lens of electron gun |
US07/013,676 US4800318A (en) | 1986-02-12 | 1987-02-12 | Electrode assembly for electrostatic lens of electron gun |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61214431A JP2570700B2 (en) | 1986-09-10 | 1986-09-10 | Electron gun electrode assembly |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6369128A JPS6369128A (en) | 1988-03-29 |
JP2570700B2 true JP2570700B2 (en) | 1997-01-08 |
Family
ID=16655668
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61214431A Expired - Lifetime JP2570700B2 (en) | 1986-02-12 | 1986-09-10 | Electron gun electrode assembly |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2570700B2 (en) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2772429B2 (en) * | 1989-03-22 | 1998-07-02 | スズキ株式会社 | Mounting structure of bumper |
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 |
JP5662038B2 (en) * | 2010-03-03 | 2015-01-28 | 日東電工株式会社 | Patches and patch preparations |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
ZA824780B (en) * | 1981-07-10 | 1983-05-25 | Rca Corp | Color image display systems |
US4388552A (en) * | 1981-07-10 | 1983-06-14 | Rca Corporation | Color picture tube having an improved expanded focus lens type inline electron gun |
JPS5864740A (en) * | 1981-10-12 | 1983-04-18 | Nec Corp | Electron-gun electrode structure |
JPS6119030A (en) * | 1984-07-04 | 1986-01-27 | Mitsubishi Electric Corp | Electron gun |
-
1986
- 1986-09-10 JP JP61214431A patent/JP2570700B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS6369128A (en) | 1988-03-29 |
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