JPS6081743A - Flat type color cathode-ray tube device - Google Patents

Flat type color cathode-ray tube device

Info

Publication number
JPS6081743A
JPS6081743A JP19015583A JP19015583A JPS6081743A JP S6081743 A JPS6081743 A JP S6081743A JP 19015583 A JP19015583 A JP 19015583A JP 19015583 A JP19015583 A JP 19015583A JP S6081743 A JPS6081743 A JP S6081743A
Authority
JP
Japan
Prior art keywords
deflection
magnetic core
ray tube
pole magnet
adjusted
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
JP19015583A
Other languages
Japanese (ja)
Inventor
Sakae Tanaka
栄 田中
Toshio Oboshi
敏夫 大星
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.)
Sony Corp
Original Assignee
Sony 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 Sony Corp filed Critical Sony Corp
Priority to JP19015583A priority Critical patent/JPS6081743A/en
Publication of JPS6081743A publication Critical patent/JPS6081743A/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
    • H01J29/72Arrangements for deflecting ray or beam along one straight line or along two perpendicular straight lines
    • H01J29/76Deflecting by magnetic fields only

Landscapes

  • Cathode-Ray Tubes And Fluorescent Screens For Display (AREA)

Abstract

PURPOSE:To remove one-axis directional mislanding without requiring any power consumption by segmenting the annularity of an annular magnetic core for a deflection means and providing a columnar two-pole magnet in this segmentation section so as to be rotated and adjusted. CONSTITUTION:The nearly intermediate section of one-sided side section 8c of an annular magnetic core 8 that centers around the external surface of the tube body 2 of a deflection means 7 is segmented and a plastic holder 15 that is provided with a cylindrical two-pole magnet 14 so as to be rotated and adjusted is fit to this segmentation section. The number of magnetic fluxes applied in the magnetic core 8 and the bias magnetic field between the center poles 8a and 8b of the magnetic core 8 can be adjusted by rotating the adjusting the cylindrical two-pole magnet 14. As a result, this cylindrical two-pole magnet 14 can be rotated and adjusted and the one-axis directional mislanding generated when a flat type cathode-ray tube device is manufactured by adjusting a double pole magnet 12 can be removed.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は携帯用の小形力ラーテレビノヨン受像機に使用
して好適な扁平型カラー陰極線管装置に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a flat color cathode ray tube device suitable for use in a small portable color television receiver.

背景技術とその問題点 先に携帯用の小形カラーテレビジョン受像機に使用する
扁平型カラー陰極線管装置として第1図、第2図及び第
3図に示す如きものが提案されている。
BACKGROUND ART AND PROBLEMS Previously, flat color cathode ray tube devices as shown in FIGS. 1, 2 and 3 have been proposed for use in small portable color television receivers.

第1図、第2図に於いて、(1)はこの扁平型カラー陰
極線管装置を全体として示し、(2)はこの扁平型カラ
ー陰極線管装置(1)の扁平管体で、この扁平管体(2
)は例えば皿状の前面ガラス半休(2a)と、この前面
ガラス半休(2a)の周辺部に接合封着される皿状の後
面ガラス半休(2b)とより成り、両半体(2a)及び
(2b)間に扁平空間が形成されるようになされる。そ
して前面ガラス半休(2a)の内側に赤、緑及び青色を
発光する螢光体の例えばストライブ状の繰返しのカラー
螢光面(3)を設けると共にこのカラー螢光面(3)に
対応してア・ぐ−チャグリル(4)を設ける如くする。
In Figures 1 and 2, (1) shows this flat color cathode ray tube device as a whole, and (2) shows the flat tube body of this flat color cathode ray tube device (1). Body (2
) consists of, for example, a dish-shaped front glass half (2a) and a dish-shaped rear glass half (2b) that is bonded and sealed to the periphery of this front glass half (2a), and both halves (2a) and (2b) A flat space is formed between them. Then, on the inside of the front glass half-hole (2a), a color fluorescent surface (3) made of red, green, and blue light-emitting fluorescent material, such as a strip-like repeated color fluorescent surface (3), is provided, and a color fluorescent surface (3) corresponding to this color fluorescent surface (3) is provided. A gucha grill (4) is provided.

又後面ガラス半休(2b)の内側にカラー螢光面(3)
に対向して背面電極(5)を設ける。
In addition, there is a colored fluorescent surface (3) inside the rear glass half-closed (2b).
A back electrode (5) is provided opposite to.

そして、このカラー螢光面(3)の略々延長上にネック
管(2C)が設けられ、このネック管(2C)内に電子
銃(6)が収容配置される。この電子銃(6)としては
例えば1がン3ビームの所謂トリニトロン管(商品名)
と同様の構成の電子銃を使用する。
A neck tube (2C) is provided approximately on the extension of this color fluorescent surface (3), and an electron gun (6) is accommodated within this neck tube (2C). This electron gun (6) is, for example, a so-called trinitron tube (trade name) with 1 gun and 3 beams.
An electron gun with a similar configuration is used.

そして、電子銃(6)よシ発射される電子ビームを電子
銃(6)の軸心方向とほぼ直交し、且つほぼカラー螢光
面(3)の面方向に関して偏向(以下水平偏向という)
させる偏向手段と、カラー螢光面(3)と直交する方向
の偏向(以下垂直偏向という)させる偏向手段とをこの
カラー螢光面(3)と電子銃(6)との間に設ける。そ
して、この水平偏向によって、電子ビームのカラー螢光
面(3)上の水平方向走査がなされ、垂直偏向と背面電
極(5)及び中間電極とターグツト電極との電位差に基
く偏向との共働によって電子ビームの螢光面(3)上の
垂直方向走査がなされる。したがってこの場合、電子ビ
ームに対する上述の垂直偏向は、例えばその偏向角が1
0’〜200という小さい角度でよい。この電子ビーム
に対する水平偏向と垂直偏向とは、例えばその偏向角が
小さい方の垂直偏向は静電偏向によシ、またこれに比し
、大きな偏向角を必要とする水平偏向は電磁偏向による
Then, the electron beam emitted by the electron gun (6) is deflected (hereinafter referred to as horizontal deflection) approximately perpendicular to the axial direction of the electron gun (6) and approximately in the plane direction of the color fluorescent surface (3).
A deflecting means for deflecting the electron beam in a direction perpendicular to the color fluorescent surface (3) (hereinafter referred to as vertical deflection) is provided between the color fluorescent surface (3) and the electron gun (6). This horizontal deflection causes the electron beam to scan in the horizontal direction on the color phosphor surface (3), and due to the cooperation of the vertical deflection and the deflection based on the potential difference between the back electrode (5), the intermediate electrode, and the target electrode. The electron beam is scanned vertically over the fluorescent surface (3). Therefore, in this case, the above-mentioned vertical deflection to the electron beam is such that, for example, the deflection angle is 1
A small angle of 0' to 200 is sufficient. Regarding the horizontal and vertical deflections of this electron beam, for example, the vertical deflection, which has a smaller deflection angle, is caused by electrostatic deflection, while the horizontal deflection, which requires a larger deflection angle, is caused by electromagnetic deflection.

このような偏向手段としては、その水平及び垂直の両偏
向、すなわち電磁偏向と静電偏向とを共通の偏向手段(
7)によって同一位置で行う構成となし得る。この偏向
手段(7)は、例えば電子銃(6)の後段側において、
管体(2)の外周を繞って高透磁率の例えばフェライト
より成る環状の磁気コア(8)と水平偏向電流を通ずる
電磁線輪(9)と、管体(2)内に配置される高透磁率
磁性体uO)とによって構成される。
Such a deflection means includes a common deflection means (
7), it can be configured to be performed at the same location. This deflection means (7) is provided, for example, on the downstream side of the electron gun (6).
An annular magnetic core (8) made of high magnetic permeability, for example, ferrite, which surrounds the outer periphery of the tube body (2), and an electromagnetic wire ring (9) through which a horizontal deflection current passes, are arranged within the tube body (2). It is composed of a high permeability magnetic material (uO).

磁気コア(8)は、例えば第3図にその断面を示すよう
に管体(2)の外周を繞る環状となすも、管体(2)内
の電子ビームの通路を挾んで管体(2)内の高透磁率磁
性体(13の形状に対応する形状の例えば台形状の対の
センターポール(8a)及び(8b)を管体(2)の厚
さ方向に関して相対向するように内側に突出させ、これ
らセンターポール(8a)及び(8b)、或いはその何
れか一方の外周に線輪(9)を鞍型に巻装する。
For example, the magnetic core (8) has a ring shape that surrounds the outer periphery of the tube (2) as shown in the cross section of FIG. 2) A pair of trapezoidal center poles (8a) and (8b) having a shape corresponding to the shape of the tube body (2) (13) are placed inside so as to face each other in the thickness direction of the tube body (2). The center poles (8a) and (8b) are made to protrude from each other, and a wire ring (9) is wrapped around the outer periphery of the center poles (8a) and (8b) in a saddle shape.

このようにして線輪(9)に通ずる水平偏向電流に応じ
た磁束を両センター・1ソール(8a)及び(8b)間
に、すなわち管体(2)を横切って発生させ、管体(2
)内の電子ビームの通路に管体(2)の厚み方向の磁場
を与えるようにする。一方、管体(2)内の両センター
ポール(8a)及び(8b)間において、電子ビームの
通路に臨んで高透磁率体OI])が配置される。この高
透磁率体(II)は電子ビームの通路を挾んで管体(2
)の厚み方向に関する両側に相対向し、螢光面(3)側
に向って夫々広がる対の例えば台形板状高透磁率体(1
0a)及び(10b)より成り、これらによってセンタ
ーポール(8a)及び(8b)間の磁束を電子ビームの
通路に集中させる。この場合センターポールの形状を、
高透磁率体の形状に、この場合には台形にしたので、効
率良く磁束を集中させることができる。また、これら対
の高透磁率体(10a)及び(10b)は高比抵抗を有
するも電気伝導性のある例えば104〜1070備程度
の比抵抗を有する高透磁率体、例えばフェライトより構
成する。そして、これら対の高透磁率体(10a)及び
(10b)を電子ビームに対する上述の垂直偏向を行う
静電偏向板となす。すなわち、両高透磁率体(10a)
及び(iob)よシ夫々端子を導出し、両者間に垂直偏
向電圧を印加する。尚、この場合偏向手段(7)は、電
子銃(6)の後段側、すなわち高圧側に配置するので、
両静電偏向板となる両高透磁率体(10a)及び(10
b)には陽極電圧の例えば5KVが与えられ、これに垂
直偏向電圧が重畳して与えられる。又図に於いてα0は
電子銃(6)の主レンズに対応しネック管(2c)の外
周に設けられたローテーションコイル、(l渇及ヒo■
は夫々このローテーションコイルQl)の前後に設けら
れだビユリティ補正用の二重極マグネット及び四重極マ
グネットである。
In this way, a magnetic flux corresponding to the horizontal deflection current flowing through the wire ring (9) is generated between the two center soles (8a) and (8b), that is, across the tube body (2).
) to apply a magnetic field in the thickness direction of the tube (2) to the path of the electron beam. On the other hand, a high magnetic permeability material OI]) is placed between both center poles (8a) and (8b) in the tube body (2), facing the path of the electron beam. This high magnetic permeability material (II) is sandwiched between the electron beam path and the tube body (2).
) for example, a pair of trapezoidal plate-shaped high magnetic permeability materials (1
0a) and (10b), which concentrate the magnetic flux between the center poles (8a) and (8b) on the path of the electron beam. In this case, the shape of the center pole is
Since the shape of the high magnetic permeability material is trapezoidal in this case, the magnetic flux can be concentrated efficiently. Further, these pairs of high magnetic permeability materials (10a) and (10b) are made of high magnetic permeability material, such as ferrite, which has a high specific resistance and is electrically conductive, for example, a specific resistance of about 104 to 1070. These pairs of high magnetic permeability bodies (10a) and (10b) serve as electrostatic deflection plates that perform the above-mentioned vertical deflection of the electron beam. That is, both high magnetic permeability bodies (10a)
and (iob), and a vertical deflection voltage is applied between them. In this case, since the deflection means (7) is arranged on the rear side of the electron gun (6), that is, on the high pressure side,
Both high magnetic permeability bodies (10a) and (10
In b), an anode voltage of, for example, 5 KV is applied, and a vertical deflection voltage is superimposed thereon. In the figure, α0 corresponds to the main lens of the electron gun (6), and is a rotation coil installed around the outer periphery of the neck tube (2c).
are a dipole magnet and a quadrupole magnet for utility correction, which are provided before and after this rotation coil Ql), respectively.

上述したように、電子ビームの互にほぼ直交する方向の
偏向、すなわち水平及び垂直偏向の一方を電磁偏向、他
方を静電偏向によって行うことによって、例えば偏向角
の大きい水平偏向に関しては電磁偏向によって行い、偏
向角が小さく偏向歪の問題が殆んど生じない垂直方向に
関しては静電偏向によるので、従来のように両方向の偏
向を電磁偏向によるものに比しては装置が簡単小型化さ
れ、また、両方向の偏向を静電偏向によるものに比して
は、偏向歪の小さい偏向を行うことができる。
As mentioned above, by deflecting the electron beam in mutually orthogonal directions, that is, by performing one of the horizontal and vertical deflections by electromagnetic deflection and the other by electrostatic deflection, for example, horizontal deflection with a large deflection angle is performed by electromagnetic deflection. In the vertical direction, where the deflection angle is small and there is almost no problem with deflection distortion, electrostatic deflection is used, so the device can be easily miniaturized compared to conventional methods that use electromagnetic deflection for deflection in both directions. Further, compared to deflection in both directions using electrostatic deflection, deflection can be performed with smaller deflection distortion.

そして、電磁偏向手段において、高透磁率体GO)を管
体(2)内に配置して、電子ビームの通路に磁束を集中
させるようにしたので、線輪(9)が配置された磁気コ
ア(8)を管体(2)外に配した場合において、管体(
2)を横切る磁束を発生させる例えばセンターポール(
8a)及び(8b)間の間隔が犬となっても電子ビーム
通路への磁束密度を高めることができるので、その効率
を高めることができる。
In the electromagnetic deflection means, a high magnetic permeability material GO) is arranged in the tube body (2) to concentrate magnetic flux on the path of the electron beam, so that the magnetic core on which the wire ring (9) is arranged. When (8) is placed outside the tube (2), the tube (
2) For example, a center pole (
Even if the spacing between 8a) and (8b) is narrow, the magnetic flux density to the electron beam path can be increased, thereby increasing its efficiency.

更に上述したように高透磁率体(10a)及び(1ob
)を垂直偏向の静電偏向板として用いるときは、更に構
造の簡潔化をはかることができ、水平、垂直の両偏向を
同一位置にしたことと相俟って、よシ小型化の向上をは
かることができる。
Furthermore, as mentioned above, high magnetic permeability materials (10a) and (1ob
) can be used as an electrostatic deflection plate for vertical deflection, the structure can be further simplified, and together with the fact that both horizontal and vertical deflection are in the same position, it is possible to further improve miniaturization. It can be measured.

ところで斯る扁平型カラー陰極線管装置(1)に於いて
は、その製造する場合にカラー螢光面(3)の作成と、
電子銃(6)に於ける電子ビーム源の組み立て精度のず
れ等の原因で一軸方向性のミスラングングを発生する。
By the way, when manufacturing such a flat type color cathode ray tube device (1), there are two steps:
Uniaxial misranging occurs due to deviations in assembly precision of the electron beam source in the electron gun (6).

従来斯る製造する場合の一軸方向性のミスランデングを
取シ除くのに磁気コア(8)のセンターポール(8a)
 (8b)の巻装された電磁線輪(9)に所定のバイア
ス電流を供給して所定の・々イアス磁界を発生させると
共に二重極マグネット(1りを調整して行つていた。
The center pole (8a) of the magnetic core (8) is used to eliminate mislanding of uniaxial direction in conventional manufacturing.
A predetermined bias current was supplied to the wound electromagnetic wire ring (9) (8b) to generate a predetermined bias magnetic field, and the dipole magnet (1) was adjusted.

然しなから斯る一軸方向性のミスランデングを除去する
のに所定のバイアス電流を電磁線輪(9)に流す必要が
あり、携帯用の電池を使用した小形カラーテレビノヨン
受像機に於いてはそれだけ消費電力が大きくなるので不
適当であった。
However, in order to eliminate such uniaxial mislanding, it is necessary to apply a predetermined bias current to the electromagnetic wire ring (9), and in a small color TV Noyon receiver using a portable battery, This was inappropriate because the power consumption increased accordingly.

発明の目的 本発明は斯る点に鑑み上述の如く一軸方向性のミスラン
デングを電力消費をすることなく取シ該くことを目的と
する。
OBJECTS OF THE INVENTION In view of the above, an object of the present invention is to eliminate uniaxial mislanding as described above without consuming power.

発明の概要 本発明はカラー螢光面の略々延長上に位置する電子銃と
、このカラー螢光面と対向する背面電極と、このカラー
螢光面及び電子銃の間に位置する管体外周に配される環
状磁気コアを有する偏向手段とを有する扁平型カラー陰
極線管装置に於いて、この偏向手段の環状磁気コアの環
状を分断し、この分断部に柱状二極マグネットを回転調
整可能に設けたもので、斯る本発明に依れば柱状二極マ
グネットの回転調整によシ所定のバイアス磁界を発生す
ることができ一軸方向性のミスランデングを電力消費を
することなく取シ除くことができる。
Summary of the Invention The present invention provides an electron gun located approximately on an extension of a color fluorescent surface, a back electrode facing the color fluorescent surface, and an outer periphery of a tube located between the color fluorescent surface and the electron gun. In a flat color cathode ray tube device having a deflection means having an annular magnetic core disposed in the deflection means, the annular shape of the annular magnetic core of the deflection means is divided, and a columnar dipole magnet can be rotatably adjusted in the divided portion. According to the present invention, a predetermined bias magnetic field can be generated by adjusting the rotation of the columnar bipolar magnet, and uniaxial mislanding can be removed without consuming power. I can do it.

実施例 壜lTgイg−%−、f; j Jテを1乙できら百云
q訂ぞ型カラー陰極線管装置の一実施麿につき説til
l u支う。この第4図〜第8図に於いて第1図〜第3
図に対応する部分には同一符号を付し、その詳細説明を
省略する。
Example 1 Tg Ig-%-, f;
Lu support. In this figure 4 to figure 8, figure 1 to figure 3
Portions corresponding to the figures are given the same reference numerals, and detailed explanation thereof will be omitted.

本例に於いては第4図及び第5図に示す様に第1図及び
第2図に示す扁平型カラー陰極線管装置(1)の偏向手
段(力の管体(2)の外周を繞る環状磁気コア(8)の
一方の側部(8c)の略中間部を分断し、この分断部に
第6図に示す如き円柱状二極マグネットIを回転調整可
能に配したシラスチックホルダ+151を装着する。そ
の他は第1図及び第2図に示す如く構成する。
In this example, as shown in FIGS. 4 and 5, the deflection means (which covers the outer periphery of the force tube (2)) of the flat color cathode ray tube device (1) shown in FIGS. 1 and 2 is used. A silastic holder +151 in which an annular magnetic core (8) is divided approximately in the middle of one side (8c), and a cylindrical bipolar magnet I as shown in FIG. 6 is rotatably arranged in this divided part. The other parts are constructed as shown in FIGS. 1 and 2.

本例に於いては第8図A、B及びCに示す如く円柱状二
極マグネット(14)を回転調節することに依り磁気コ
ア(8)内を流れる磁束数を調整でき、磁気コア(8)
のセンターポール(8a)及び(8b)間に発生するバ
イアス磁界を調整できる。従ってこの円柱状二極マグネ
ット0滲を回転調整すると共に二重極マグネット0りを
調整して扁平型カラー陰極線管装置の製造時に生ずる一
軸方向性のミスランデングを取り除くことができる。斯
る構成に依れば円柱状二極マグネットI及び二重極マグ
ネット(1りにょシー軸方向性のミスランデングを取り
除く様にしているので消費電力が零で、この−軸方向性
ミスランデングを取り除くことができる。又本例に於い
ても第1図及び第2図に示す如き扁平型カラー陰極線管
装置の作用効果が得られることは勿論である。
In this example, the number of magnetic fluxes flowing in the magnetic core (8) can be adjusted by adjusting the rotation of the cylindrical bipolar magnet (14) as shown in FIGS. 8A, B, and C. )
The bias magnetic field generated between the center poles (8a) and (8b) can be adjusted. Therefore, by rotating and adjusting the rotation of this cylindrical dipole magnet and adjusting the rotation of the dipole magnet, it is possible to eliminate uniaxial mislanding that occurs when manufacturing a flat color cathode ray tube device. According to this configuration, the power consumption is zero because mislanding in the axial direction of the cylindrical bipolar magnet I and the bipolar magnet (1) is removed. It goes without saying that this embodiment also provides the effects of the flat color cathode ray tube device as shown in FIGS. 1 and 2.

尚本発明は上述実施例に限ることなく本発明の要旨を逸
脱することなく、その他種々の構成が取り得ることは勿
論である。
It goes without saying that the present invention is not limited to the above-described embodiments, and that various other configurations can be taken without departing from the gist of the present invention.

発明の効果 本発明に依れば柱状二極マグネットの回転調整によシ所
定のバイアス磁界を発生することができ一軸方向性のミ
スランデングを電力消費をすることなく取り除くことが
でき、本発明を電池を使用した携帯用のカラーテレビジ
ョン受像機に使用して極めて有利である。
Effects of the Invention According to the present invention, a predetermined bias magnetic field can be generated by adjusting the rotation of a columnar dipole magnet, and mislanding in uniaxial direction can be removed without consuming power. It is extremely advantageous for use in portable color television receivers that use batteries.

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

第1図は扁平型カラー陰極線管の例を示す平面図、第2
図は第1図の縦方向中央断面図、第3図は第1図のIn
 −I[1線断面図、第4図は本発明扁平型カラー陰極
線管の一実施例の要部の断面図、第5図は本発明に使用
される磁気コアの例を示す斜視図、第6図は柱状二極マ
グネットの例を示す斜視図、第7図はグラスチックホル
ダの例を示す斜視図、第8図は本発明の説明に供する線
図である。 (2)は扁平管体、(3)はカラー螢光面、(5)は背
面電極、(6)は電子銃、(7)は偏向手段、(8)は
環状磁気コア、(121は二重極マグネット、uは円柱
状二極マグネットである。
Figure 1 is a plan view showing an example of a flat color cathode ray tube;
The figure is a longitudinal center sectional view of Figure 1, and Figure 3 is the In
-I[1-line sectional view, FIG. 4 is a sectional view of essential parts of an embodiment of the flat color cathode ray tube of the present invention, and FIG. 5 is a perspective view showing an example of the magnetic core used in the present invention. 6 is a perspective view showing an example of a columnar bipolar magnet, FIG. 7 is a perspective view showing an example of a plastic holder, and FIG. 8 is a diagram for explaining the present invention. (2) is a flat tube, (3) is a color fluorescent surface, (5) is a back electrode, (6) is an electron gun, (7) is a deflection means, (8) is an annular magnetic core, (121 is a double The heavy pole magnet, u, is a cylindrical dipole magnet.

Claims (1)

【特許請求の範囲】[Claims] カラー螢光面の略々延長上に位置する電子銃と、上記カ
ラー螢光面と対向する背面電極と、上記カラー螢光面及
び上記電子銃の間に位置する管体外周に配される環状磁
気コアを有する偏向手段とを有する扁平型カラー陰極線
管装置に於いて、上記偏向手段の環状磁気コアを分断し
、該分断部に柱状二極マグネットを回転詞整可能に設け
たことを特徴とする扁平型カラー陰極線管装置。
an electron gun located approximately on an extension of the color fluorescent surface, a back electrode facing the color fluorescent surface, and an annular shape disposed on the outer periphery of the tube located between the color fluorescent surface and the electron gun. A flat color cathode ray tube device having a deflection means having a magnetic core, characterized in that the annular magnetic core of the deflection means is divided, and a columnar dipole magnet is provided in the divided portion so as to be rotatable. A flat color cathode ray tube device.
JP19015583A 1983-10-12 1983-10-12 Flat type color cathode-ray tube device Pending JPS6081743A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19015583A JPS6081743A (en) 1983-10-12 1983-10-12 Flat type color cathode-ray tube device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19015583A JPS6081743A (en) 1983-10-12 1983-10-12 Flat type color cathode-ray tube device

Publications (1)

Publication Number Publication Date
JPS6081743A true JPS6081743A (en) 1985-05-09

Family

ID=16253332

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19015583A Pending JPS6081743A (en) 1983-10-12 1983-10-12 Flat type color cathode-ray tube device

Country Status (1)

Country Link
JP (1) JPS6081743A (en)

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