JPS58111244A - Color picture tube - Google Patents

Color picture tube

Info

Publication number
JPS58111244A
JPS58111244A JP20937081A JP20937081A JPS58111244A JP S58111244 A JPS58111244 A JP S58111244A JP 20937081 A JP20937081 A JP 20937081A JP 20937081 A JP20937081 A JP 20937081A JP S58111244 A JPS58111244 A JP S58111244A
Authority
JP
Japan
Prior art keywords
magnetic field
deflection magnetic
deflecting
deflection
horizontally
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP20937081A
Other languages
Japanese (ja)
Inventor
Mamoru Sakai
酒井 衛
Kiyoshi Tokita
清 時田
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura 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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP20937081A priority Critical patent/JPS58111244A/en
Publication of JPS58111244A publication Critical patent/JPS58111244A/en
Pending 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
    • H01J29/70Arrangements for deflecting ray or beam
    • H01J29/701Systems for correcting deviation or convergence of a plurality of beams by means of magnetic fields at least
    • H01J29/707Arrangements intimately associated with parts of the gun and co-operating with external magnetic excitation devices

Abstract

PURPOSE:To reduce coma aberrations to a practically permissible degree by providing magnetically-high-resistance parts at parts which are practically parallel to the horizontally-deflecting magnetic fields of deflecting-magnetic-field controlling elements and vertical to the horizontal axis. CONSTITUTION:Magnetically-high-resistance parts 18, 19, 22 and 23 are provided at part, which are practically parallel to the horizontally-deflecting magnetic fields of deflecting-magnetic-field controlling elements 15 and 16 and include the centers of both side-beam discharging holes 12 and 14. Owing to such a constitution, most of the magnetic flux of a horizontally-deflecting magnetic field which is to pass near the center of a center-beam discharging hole 13 is absorbed by deflecting-magnetic-field controlling elements 20 and 21, and the intensity of the horizontally-deflecting magnetic field is weakened. In addition, horizontally-deflecting magnetic fields which are to pass near the holes 12 and 14 are absorbed by deflecting magnetic-field controlling elements 17, 20, 21 and 24. Consequently, the elements 15 and 16 decrease the horizontally deflected sensitivity of a center beam, increase the horizontally deflected sensitivities of both side electron beams, and can correct the side coma aberration among the coma aberrations of a pattern projected upon a picture screen.

Description

【発明の詳細な説明】 発明の技術分野 本発明はインライン配列3電子銃を有するカラー受像管
の、特に偏向磁界制御素子によるビン歪補正量を軽減す
るカラー受像管に関するものである。
TECHNICAL FIELD OF THE INVENTION The present invention relates to a color picture tube having an in-line arrangement of three electron guns, and particularly to a color picture tube that reduces the amount of bin distortion correction by a deflection magnetic field control element.

発明の技術的背景と問題点 インライン配列3電子銃を有するカラー受像管では赤、
縁及び青の各専用電子銃による画面上での偏向走査領域
(以下パターンと称す)の歪や一致度が問題となる0画
面水平軸に沿って一列に配列され九インライン配列3電
子銃による電子ビームは外部からの偏向手段即ち、水平
軸に平行な方向の垂直偏向磁界と水平軸に垂直な方向の
水平偏向磁界忙よ抄偏−向走査されるが、中央電子ビー
ムと両サイド電子ビームのパターン歪や一致度が最も重
要である。第1Iaは4Hcインツイン配列3電子銃を
収納していゐネック部の断面の各偏向磁界分布を示すも
ので、水平偏向磁界(1)をビyクツシヲン磁界に垂直
偏向磁界(2)をバレル磁界にすることにより両サイド
電子ビーム関の色ずれを減少させてお妙受像機側のコン
バーゼンス回路が単純化される利点がある。しかし乍ら
2勢の偏向磁界は何れも非斉一磁界分布であプ、中央電
子ビーム(4)K対する偏向感度が両サイド電子ビーム
(3)及び(5)に対する偏向感度よ)悪くなる欠点を
有している。
Technical Background and Problems of the Invention In a color picture tube with an in-line array of three electron guns, red,
Deflection and consistency of the deflection scanning area (hereinafter referred to as pattern) on the screen by each of the edge and blue dedicated electron guns is a problem.0 The electrons are arranged in a line along the horizontal axis of the screen, and the electrons are arranged in nine in-line arrays by three electron guns. The beam is deflected and scanned by external deflection means, that is, a vertical deflection magnetic field parallel to the horizontal axis and a horizontal deflection magnetic field perpendicular to the horizontal axis. Pattern distortion and degree of matching are most important. 1Ia shows the deflection magnetic field distribution in the cross section of the neck section housing the 4Hc in-twin array 3 electron gun. This has the advantage of reducing color shift between the electron beams on both sides and simplifying the convergence circuit on the receiver side. However, both of the two deflection magnetic fields have a non-uniform magnetic field distribution, which has the disadvantage that the deflection sensitivity for the central electron beam (4) K is worse than the deflection sensitivity for the side electron beams (3) and (5). have.

この場合画面上には第2図に示すような両サイド電子ビ
ームによるパターン(6)と中央電子ンー五によるパタ
ーン(7)が得られ、このようfk現象はコマ収差のあ
る状態と見做される。
In this case, a pattern (6) due to both side electron beams and a pattern (7) due to central electron beams as shown in Fig. 2 are obtained on the screen, and this fk phenomenon is considered to be a state with coma aberration. Ru.

これを補正する為に従来は第3図に示すような磁性体か
らなる偏向磁界制御素子を電子銃の電子ビーム放出孔に
1通常は電子銃最先端(蛍光面側)の電極底部に設けて
いる。第3図に於て1両サイド電子ビーム放出孔(2)
及びa4を取り囲むように設けられた磁性体(8)及び
(9)からなる偏向磁界制御素子は水平及び垂直画偏向
磁界を弱め、中央電子ビーム放出孔付近の垂直偏向磁界
を強めるように働く、一方中央電子ビーム放出孔(2)
の水平軸に対して上下@に設けられた磁性体tlI及び
αυからなる偏向磁界制御素子は中央電子ビーム放出孔
付近の水平偏向磁界を強めるように慟く。この結釆絢す
イド電子ビーム九対する偏向感度が中央電子ビームに対
する偏向感度よシも急くなり、非斉一な偏向磁界による
中央電子ビームの偏向感度の劣化を補正し画面上にはコ
マ収差の少ないパターンが得られる。
In order to correct this, conventionally, a deflection magnetic field control element made of a magnetic material as shown in Figure 3 was installed in the electron beam emission hole of the electron gun, usually at the bottom of the electrode at the tip of the electron gun (on the phosphor screen side). There is. In Figure 3, one side electron beam emission hole (2)
and a deflection magnetic field control element consisting of magnetic bodies (8) and (9) provided so as to surround a4, which functions to weaken the horizontal and vertical image deflection magnetic fields and strengthen the vertical deflection magnetic field near the central electron beam emission hole; On the other hand, the central electron beam emission hole (2)
A deflection magnetic field control element consisting of magnetic bodies tlI and αυ provided above and below with respect to the horizontal axis of the electron beam is controlled to strengthen the horizontal deflection magnetic field near the central electron beam emission hole. As a result, the deflection sensitivity for the nine id electron beams becomes faster than the deflection sensitivity for the center electron beam, which compensates for the deterioration in the deflection sensitivity of the center electron beam due to the non-uniform deflection magnetic field, resulting in less comatic aberration on the screen. A pattern is obtained.

ところで受像機側でコンバーゼンス補正回路を省略しよ
うとしたり、ビンクッション歪補正量を軽減しようとし
て偏向ヨークの楕類や磁界分布を種々変化させ′ると上
記目標を達成することのできる偏向ヨークとカラー受像
管の組み合せに対してコマ収差のパターンは必らずしも
第2図に示すようなパターンではなく第4図のようなパ
ターンとなゐ場合がある。即ち、両ナイド電子ビームに
よるパターン(6)と中央電子ビームによるパターン(
7)が入り組んだ状態となり、このよう表パターンの場
合は第3図のような偏向磁界制御素子ではコマ収差の軽
減に対応することは出来ない。
By the way, if you try to omit the convergence correction circuit on the receiver side or try to reduce the amount of bin cushion distortion correction by variously changing the ellipse of the deflection yoke and the magnetic field distribution, you will be able to find a deflection yoke and collar that can achieve the above goals. The pattern of comatic aberration for a combination of picture tubes is not necessarily a pattern as shown in FIG. 2, but may be a pattern as shown in FIG. 4. That is, the pattern (6) due to both side electron beams and the pattern (6) due to the center electron beam
7) becomes complicated, and in the case of such a front pattern, the deflection magnetic field control element as shown in FIG. 3 cannot reduce the coma aberration.

発明の目的 本発明は以上の点に鑑みてなされたもので、コマ収差管
実用上許容し得るようVC@滅したカラー受像管を提供
せんとすることにある。
OBJECTS OF THE INVENTION The present invention has been made in view of the above points, and it is an object of the present invention to provide a color picture tube in which VC@ is eliminated so that the coma aberration tube is practically acceptable.

本発明の目的は両サイド電子ビームに対する偏向感度と
中央電子ビームに対する偏向感度が異なるカラー受像管
と偏向冒−りの組み合せに対して両サイド電子ビームと
中央電子ビームに対する偏向感度の差を解消する手段を
提供することkある。
The purpose of the present invention is to solve the difference in the deflection sensitivity between the two side electron beams and the center electron beam in a combination of a color picture tube and a deflection sensor, which have different deflection sensitivities for the two side electron beams and the center electron beam. There is a need to provide means.

発明の概要 本発明は水平軸に8って一列に配列されたインツイン配
列3電子銃を有し、電子ビームが水平軸に垂直な方向の
水平偏向磁界と、水平軸に平行な方向の垂直偏向磁界に
より偏向走査され、両サイドビーム通過領域を包囲する
ように配設された偏向磁界制御素子を有するカラー受像
管において、偏向磁界制御素子の両サイドビームの各々
の中心を含む水平軸忙垂直々部分に磁気的に高抵抗な部
分を設けるととによって、偏向磁界の実効強度分布を変
化させ両サイド電子ビームに対する偏向磁界強度と中央
電子ビームに対する偏向磁界とを互に異らせて上記目的
を達成するものである。
SUMMARY OF THE INVENTION The present invention has an in-twin array three electron guns arranged in a row on a horizontal axis, and the electron beam is deflected by a horizontal deflection magnetic field in a direction perpendicular to the horizontal axis and a vertical deflection field in a direction parallel to the horizontal axis. In a color picture tube which is deflected by a deflection magnetic field and has a deflection magnetic field control element disposed so as to surround both side beam passing areas, the horizontal axis including the center of each of the both side beams of the deflection magnetic field control element is vertical. The effective intensity distribution of the deflection magnetic field is changed by providing magnetically high resistance sections in each section, thereby making the deflection magnetic field strength for both side electron beams and the deflection magnetic field for the center electron beam different from each other, thereby achieving the above-mentioned purpose. The goal is to achieve the following.

発明の実施例 以下に実施例をあけて本発明の詳細な説明する。Examples of the invention The present invention will be described in detail below with reference to Examples.

第5図は本発明のカラー受像管に適用される偏向磁界制
御素子(6)及び(6)を蛍光面側から見た正面図であ
る。第5図に示す偏向磁界制御素子(ト)及び(至)は
偏向磁界の及ぶ領域、例えばインライン配列3電子銃の
蛍光面側最先端の電極底部に配置されるが、ここでは電
極を含めた全体は省略し要部のみを示しである。第5図
に於て電子ビーム放出孔Qal(至)及びα◆は水平軸
線[5って一直線状に配設されている。そして両サイド
ビーム放出孔(ロ)及び(ロ)即ち両サイドビーム通過
領域を包囲すゐように偏向磁界制御素子(至)及び(2
)が設けられている。
FIG. 5 is a front view of the deflection magnetic field control elements (6) and (6) applied to the color picture tube of the present invention, viewed from the phosphor screen side. The deflection magnetic field control elements (g) and (to) shown in Fig. 5 are placed in the area covered by the deflection magnetic field, for example, at the bottom of the most advanced electrode on the phosphor screen side of the in-line array 3 electron gun. The whole is omitted and only the main parts are shown. In FIG. 5, the electron beam emission hole Qal (to) and α◆ are arranged in a straight line along the horizontal axis [5]. Then, the deflection magnetic field control elements (to) and (2) are arranged so as to surround both side beam emission holes (b) and (b), that is, both side beam passage areas.
) is provided.

この偏向磁界制御素子(至)及び輔の水平偏向磁界と実
質的に平行であって、両サイドビーム放出孔の各々の中
心を含む水平軸KfllI[fk部分には磁気的に高抵
抗な部分QI、(6)、@及び(2)が設けられている
The horizontal axis KfllI [fk portion is substantially parallel to the horizontal deflection magnetic field of the deflection magnetic field control element (to) and the horizontal deflection magnetic field of , (6), @ and (2) are provided.

第5図に示すように偏向磁界制御素子を構成するととK
よって、本来中央ビーム放出孔側の中心付近を通るべき
水平偏向磁界の磁束の多くは偏向磁界制御素子員及び@
によって吸収され、中央ビーム放出孔付近の水平偏向磁
界強度は磁界制御素子がない場合に比べて弱くなる。
If the deflection magnetic field control element is configured as shown in FIG.
Therefore, most of the magnetic flux of the horizontal deflection magnetic field, which should originally pass near the center on the side of the central beam emission hole, flows through the deflection magnetic field control element members and @
, and the horizontal deflection magnetic field strength near the central beam emission hole becomes weaker than when there is no magnetic field control element.

また本来両サイドビーム放出孔(2)及び(ロ)の近辺
を通るべき水平偏向磁界は偏向磁界制御素子Q7)。
Also, the horizontal deflection magnetic field that should originally pass near both side beam emission holes (2) and (b) is the deflection magnetic field control element Q7).

翰、@及び(24によって吸収される。Absorbed by Kan, @ and (24).

しかし本来両サイドビーム放出孔(至)及び(ロ)の中
心付近を通るべき水平偏向磁界の磁束の一部は磁気的に
高抵抗な部分w、011.@及び−の偏向磁界制御素子
部分を通過し、両サイドビーム孔の中心付近を通ること
になる。
However, a part of the magnetic flux of the horizontal deflection magnetic field that should originally pass near the center of both side beam emission holes (to) and (b) is a magnetically high resistance part w, 011. It passes through the @ and - deflection magnetic field control element parts, and passes near the center of both side beam holes.

従って偏向磁界制御素子(至)、 (40、@及び(至
)が磁気的に高抵抗である場合の方が両サイドビーム放
出孔付近における磁束は強い。従って偏向磁界制御素子
(2)及び(ト)は結果として中央ビームの水平偏向感
度を弱め1両サイド電子ビームの水平偏向感度を強める
働きをし、第4図に示すようなパターンのコマ収差のう
ち左右のコマ収差を補正することができる。−この場合
の偏向磁界制御素子(至)及び@による水平偏向磁界強
度の分布特性を第1図に示す、第7図に於て横軸は谷電
子ビーム放出孔(6)。
Therefore, when the deflection magnetic field control elements (to), (40, @ and (to) have high magnetic resistance, the magnetic flux near both side beam emission holes is stronger. Therefore, the deflection magnetic field control elements (2) and (40, @ and (to) As a result, the horizontal deflection sensitivity of the central beam is weakened, and the horizontal deflection sensitivity of the electron beams on both sides is strengthened, and it is possible to correct the left and right coma aberrations in the pattern shown in Figure 4. - The distribution characteristics of the horizontal deflection magnetic field intensity due to the deflection magnetic field control element (to) and @ in this case are shown in FIG. 1. In FIG. 7, the horizontal axis is the valley electron beam emission hole (6).

(至)及び(ロ)に対応する中心位置6υ、に)及び−
を夫々示し、縦軸は水平偏向磁界強度(BH)を示す。
To the center position 6υ corresponding to (to) and (b)) and -
are shown, respectively, and the vertical axis shows the horizontal deflection magnetic field strength (BH).

偏向磁界制御素子そのものがない場合の水平偏向磁界強
度分布−と、両サイドビームの偏向磁界制御素子が第3
図に示す場合の水平偏向磁界強度分布(2)に対して、
本発明の実施例の場合の水平偏向磁界強度分布竺の差が
明確に示されている。
Horizontal deflection magnetic field strength distribution when there is no deflection magnetic field control element itself, and when the deflection magnetic field control element of both side beams is the third
For the horizontal deflection magnetic field strength distribution (2) in the case shown in the figure,
The difference in the horizontal deflection magnetic field intensity distribution in the case of the embodiment of the present invention is clearly shown.

館6図は本発明の他の実施例を示すもので、第5図の実
施例に加えて、#j4Ii[偏向磁界と実質的和平性で
両サイドビームの水平中心軸に対して中央ビーム放出孔
とは反対側の部分に磁気的に高抵抗な偏向磁界制御素子
部分(2)及び四を設けたものである。
Figure 6 shows another embodiment of the present invention, in addition to the embodiment shown in Figure 5. Magnetically high-resistance deflection magnetic field control element portions (2) and (4) are provided on the opposite side of the hole.

第6図に示すように偏向磁界制御素子を構成することに
よって1本来両サイドビーム放出孔(2)及び(141
の中心付近を通るべき垂直偏向磁界の磁束の多くは偏向
磁界制御素子部分(ホ)、@、@、(支)、(2)及び
■によって吸収され、両サイドビーム放出孔付近の垂直
偏向磁界の磁束が少くなり、一方中央ビーム放出孔の中
心付近の垂直偏向磁界の磁束は強くなる。従って両サイ
ドビームの垂直偏向感度を弱め、中央電子ビームOII
直偏向感度を強める働きをし、第4図に示すようなパタ
ーンのコマ収差のうち上下のコマ収差を補正することが
できる。
By configuring the deflection magnetic field control element as shown in FIG.
Most of the magnetic flux of the vertical deflection magnetic field that should pass near the center of is absorbed by the deflection magnetic field control element part (E), @, @, (support), (2) and ■, and the vertical deflection magnetic field near the both side beam emission holes The magnetic flux of the vertical deflection field near the center of the central beam exit hole becomes stronger. Therefore, the vertical deflection sensitivity of both side beams is weakened, and the central electron beam OII
It works to strengthen the direct deflection sensitivity, and among the coma aberrations in the pattern shown in FIG. 4, it is possible to correct the upper and lower coma aberrations.

この場合の偏向磁界制御素子(至)及び01によゐ垂直
偏向磁界強度(Bv)0分布特性を第7図と同様の方式
で第8図に示す、第8図に於て、偏向磁界制御素子その
ものがない場合の垂直偏向磁界強度分布□□□と、偏向
磁界制御素子部分−及び(2)以外の偏向磁界制御素子
部分がない場合の接直偏向磁界強度分布@に、対して1
本発甲の実施例の場合の垂直偏向磁界強度分布員の差が
明確に示されている。
The vertical deflection magnetic field strength (Bv) 0 distribution characteristics of the deflection magnetic field control element (to) and 01 in this case are shown in FIG. 8 in the same manner as in FIG. 7. 1 for the vertical deflection magnetic field strength distribution □□□ without the element itself and the direct deflection magnetic field strength distribution @ when there is no deflection magnetic field control element part other than the deflection magnetic field control element part - and (2)
The difference in the vertical deflection magnetic field strength distribution in the case of this embodiment is clearly shown.

以上の説明に於て、第5図の実施例では主として左右の
コマ収差の補正について、第6図の実施例では主として
上下のコマ収差の補正の作用について説明したが、基本
的には第6図の実施例の場合の方が第5図の冥施例の場
合よシもより効果的にコマ収差を補正することができる
In the above explanation, in the embodiment shown in FIG. 5, the correction of left and right coma aberration was mainly explained, and in the embodiment shown in FIG. 6, the effect of correction of vertical coma aberration was mainly explained. The embodiment shown in the figure can correct comatic aberration more effectively than the embodiment shown in FIG.

尚、第5図及び第6図に示した偏向磁界制御素子の磁気
的に高抵抗な部分の一部又は全部はギャップで構成され
ていてもよく、また非磁性体で構成されていてもよい、
即ち、この磁気的に高抵抗な部分は用いる偏向ヨークと
カラー受像管の組み合せに応じてその水平及び垂直偏向
磁界強度分布を本発明の主旨に従って適宜選択設計され
るべきであゐ。
Note that part or all of the magnetically high resistance portion of the deflection magnetic field control element shown in FIGS. 5 and 6 may be formed of a gap or may be formed of a non-magnetic material. ,
That is, the horizontal and vertical deflection magnetic field strength distributions of this magnetically high resistance portion should be appropriately selected and designed according to the combination of the deflection yoke and color picture tube used, in accordance with the gist of the present invention.

発明の効果 以上のように本発明によれば、垂直偏向磁界に対する中
央ビームの偏向感度を両サイドビームの偏向感度より相
対的に増加させ、且つ水平偏向磁界に対する両サイドビ
ームの偏向感度を中央ビームの偏向感度より固相対的に
増加させることKよって、インライン配列3電子銃を有
するカラー受像管の画面上のパターyK於て1両サイド
電子ビー′五に対する中央電子ビームのパターンが水平
方向に長く垂直方向に短かいコマ収差を容易に効果的に
補正することができ、これによシコンパーゼンス補正回
路を省略しピン歪補正量を軽減することが可能となシそ
の工業的価値は大である。
Effects of the Invention As described above, according to the present invention, the deflection sensitivity of the center beam to the vertical deflection magnetic field is relatively increased compared to the deflection sensitivity of both side beams, and the deflection sensitivity of both side beams to the horizontal deflection magnetic field is increased relative to the deflection sensitivity of the center beam to the horizontal deflection magnetic field. By increasing the deflection sensitivity of K relative to the solid relative, the pattern of the central electron beam for one side electron beam '5 is lengthened in the horizontal direction in the putter yK on the screen of a color picture tube with three electron guns in an in-line arrangement. Comatic aberrations that are short in the vertical direction can be easily and effectively corrected, and the comparability correction circuit can be omitted and the amount of pin distortion correction can be reduced, which is of great industrial value.

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

第1図はネック部の偏向磁界分布を説明するための概略
断面図、第2図は第1図の偏向磁界分布による画面上パ
ターンを示す模式図、籐3図は従来の磁界制御素子を示
す概略断面図、第4図はインライン配列3電子銃を有す
るカラー受像管の画面上パターンを示す模式図、第5図
及び第6図は本発明に適用される磁界制御素子の配置の
実施例を示す概略断面図、第7図及び第8図は第5図及
び第6図の水平及び垂直偏向磁界強度を各電子ビーム位
置毎に示す分布特性図である。 (2)、α◆・・・・サイド電子ビーム放出孔(至)・
・・・中央電子ビーム放出孔 (ト)、QIS・・・・偏向磁界制御素子αη、(ホ)
、(ハ)、124.幹、鰭、(ハ)、(至)・・・・・
・偏向磁界制御素子部分 (至)、054 、 @ 、 @ 、(ホ)、翰・・・
・・磁気的高抵抗部分(7317)  代理人 弁理士
 則 近 憲 佑 (ほか1名)第1.    第3図 第2図    第4図
Figure 1 is a schematic cross-sectional view for explaining the deflection magnetic field distribution at the neck, Figure 2 is a schematic diagram showing the pattern on the screen due to the deflection magnetic field distribution in Figure 1, and Figure 3 shows a conventional magnetic field control element. A schematic cross-sectional view, FIG. 4 is a schematic diagram showing the on-screen pattern of a color picture tube having three electron guns in an in-line arrangement, and FIGS. 5 and 6 show examples of the arrangement of magnetic field control elements applied to the present invention. The schematic cross-sectional views shown in FIGS. 7 and 8 are distribution characteristic diagrams showing the horizontal and vertical deflection magnetic field intensities shown in FIGS. 5 and 6 for each electron beam position. (2), α◆・・・Side electron beam emission hole (to)・
... Central electron beam emission hole (G), QIS ... Deflection magnetic field control element αη, (E)
, (c), 124. Trunk, fin, (ha), (to)...
・Deflection magnetic field control element part (to), 054, @, @, (e), Kan...
...Magnetic high resistance part (7317) Agent: Patent attorney Noriyuki Chika (and 1 other person) 1st. Figure 3 Figure 2 Figure 4

Claims (1)

【特許請求の範囲】 1)水平軸1icfi1って一列に配列され九インライ
ン配列3電子銃を有し前記電子銃の電子ビームが前記水
平軸に喬直な方向O水平偏向磁界と前記水平軸に平行な
方向の接直偏向磁界によ)偏向走査され前記インライン
配列3電子銃のうち両サイドビーム通過領域を包囲する
ように配設された偏向磁界制御素子を有するカラー受像
管において、前記偏向磁界制御素子O前記水平偏向磁界
と実質的に平行であって前記両ナイドビームの各々の中
心を含む前記水平軸に−直な部分に磁気的に高抵抗な部
分を設は九ことを特徴とするカラー受像管。 2)偏向磁界制御素子の、前記喬直偏向磁界と実質的に
平行であって前記両ナイドビームの各々の中心を含む前
記水平軸に実質的に平行で中央ビームとは反対側の部分
に磁気的に高抵抗壜部分を設は九ことを特徴とする特許
請求の範囲第1項記載のカラー受像管。 3)磁気的に高抵抗な部分の一部又は全部がギャップか
らなることを特徴とする特許請求の範囲第1項又は第2
項記載のカラー受像管。 4)磁気的に高抵抗な部分の一部又は全部が非磁性体か
らなることを特徴とする特許請求の範囲第1項又は第2
項記載のカラー受像管。
[Claims] 1) Nine in-line array three electron guns are arranged in a row with a horizontal axis 1icfi1, and the electron beam of the electron gun is directed perpendicularly to the horizontal axis with a horizontal deflection magnetic field. In a color picture tube, the deflection magnetic field is scanned by a direct deflection magnetic field in a parallel direction and has a deflection magnetic field control element arranged so as to surround both side beam passing regions of the three in-line electron guns. A collar characterized in that a control element O is provided with a magnetically high resistance portion in a portion substantially parallel to the horizontal deflection magnetic field and perpendicular to the horizontal axis including the center of each of the two nide beams. Picture tube. 2) A portion of the deflection magnetic field control element that is substantially parallel to the perpendicular deflection magnetic field, substantially parallel to the horizontal axis including the centers of each of the two side beams, and opposite to the central beam is magnetically 2. The color picture tube according to claim 1, further comprising a high-resistance bottle portion. 3) Claim 1 or 2, characterized in that part or all of the magnetically high resistance portion consists of a gap.
Color picture tube as described in section. 4) Claim 1 or 2, characterized in that part or all of the magnetically high resistance portion is made of a non-magnetic material.
Color picture tube as described in section.
JP20937081A 1981-12-25 1981-12-25 Color picture tube Pending JPS58111244A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20937081A JPS58111244A (en) 1981-12-25 1981-12-25 Color picture tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20937081A JPS58111244A (en) 1981-12-25 1981-12-25 Color picture tube

Publications (1)

Publication Number Publication Date
JPS58111244A true JPS58111244A (en) 1983-07-02

Family

ID=16571801

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20937081A Pending JPS58111244A (en) 1981-12-25 1981-12-25 Color picture tube

Country Status (1)

Country Link
JP (1) JPS58111244A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59146131A (en) * 1983-02-09 1984-08-21 Nec Corp Inline type electron gun
JPS60262336A (en) * 1984-06-07 1985-12-25 Nec Corp Inline type electron gun
EP0243541A2 (en) * 1986-04-29 1987-11-04 Koninklijke Philips Electronics N.V. Colour television display tube with coma correction

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59146131A (en) * 1983-02-09 1984-08-21 Nec Corp Inline type electron gun
JPH0367296B2 (en) * 1983-02-09 1991-10-22 Nippon Electric Co
JPS60262336A (en) * 1984-06-07 1985-12-25 Nec Corp Inline type electron gun
EP0243541A2 (en) * 1986-04-29 1987-11-04 Koninklijke Philips Electronics N.V. Colour television display tube with coma correction

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