JPS61292840A - Color picture tube device - Google Patents

Color picture tube device

Info

Publication number
JPS61292840A
JPS61292840A JP60133966A JP13396685A JPS61292840A JP S61292840 A JPS61292840 A JP S61292840A JP 60133966 A JP60133966 A JP 60133966A JP 13396685 A JP13396685 A JP 13396685A JP S61292840 A JPS61292840 A JP S61292840A
Authority
JP
Japan
Prior art keywords
magnetic field
electron
nonsymmetrical
electron beam
electron beams
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.)
Granted
Application number
JP60133966A
Other languages
Japanese (ja)
Other versions
JP2565863B2 (en
Inventor
Taketoshi Shimoma
下間 武敏
Kumio Fukuda
福田 久美雄
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
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 filed Critical Toshiba Corp
Priority to JP60133966A priority Critical patent/JP2565863B2/en
Priority to KR1019860004958A priority patent/KR900002905B1/en
Priority to CN198686104329A priority patent/CN86104329A/en
Priority to EP86108417A priority patent/EP0207394B1/en
Priority to DE8686108417T priority patent/DE3674268D1/en
Publication of JPS61292840A publication Critical patent/JPS61292840A/en
Priority to US07/157,130 priority patent/US4845401A/en
Application granted granted Critical
Publication of JP2565863B2 publication Critical patent/JP2565863B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To produce bright images of high resolution over the entire area of the screen with a minimal strain of the electron beam spot by making three electron beams discharged from an electron gun almost parallel to each other and producing both a horizontally deflecting magnetic field which is almost homogeneous and a vertically deflecting magnetic field which is vertically symmetrical relative to the axis of a color picture tube device. CONSTITUTION:When the vertically deflecting magnetic field is vertically nonsymmetrical as shown in Fig. (a), the electron beams are deflected upward. When it is vertically nonsymmetrical as shown in Fig. (b), the electron beams are deflected downward. The distance (D) between the axis of symmetry of the magnetic field and the axis of the electron beam increases as the intensity of the nonsymmetrical deflecting magnetic field increases. That is to say, the side electron beams receive outward force which is proportional to the intensity of the nonsymmetrical magnetic field, thereby increasing the distance between the deflecting electron beams at the end of the vertical axis. It is possible to make the beam axis at the enc of the vertical axis equal to that in the center of the screen by properly selecting the intensity of the nonsymmetrical magnetic field. This nonsymmetrical magnetic field can suppress the deflectional strain of the electron beam spot to a minimal level. Besides, it is possible to prevent color shift by producing a given delay of the signal applied to the electron gun.

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形カラー受像管装置の改良に関する
DETAILED DESCRIPTION OF THE INVENTION TECHNICAL FIELD OF THE INVENTION The present invention relates to improvements in in-line color picture tube devices.

〔発明の技術的背景〕[Technical background of the invention]

カラー受像管の外囲器は3電子銃を内装するネックと、
蛍光面を有するフェースプレートと、ネックとフェース
プレートとの間に介在するファンネルとからなる。
The envelope of the color picture tube has a neck that houses three electron guns,
It consists of a face plate with a fluorescent screen and a funnel interposed between the neck and the face plate.

3電子銃はネック内に水平方向にインライン状に装着さ
れ、射出した電子ビームを蛍光体層が被着形成された蛍
光面に射突させることにより蛍光体層を発光させる6色
再現生のよい蛍光体層の発光を実現するためには、電子
ビームを選択的に所定の蛍光体層に射突させる必要があ
り、そのため多数の開孔を有するシャドウマスクがフェ
ースプレートに近接して配置される。
3. The electron gun is installed horizontally in-line inside the neck, and the emitted electron beam hits a phosphor screen on which a phosphor layer is adhered, causing the phosphor layer to emit light. In order to make the phosphor layer emit light, it is necessary to selectively impinge the electron beam on a predetermined phosphor layer, so a shadow mask with a large number of apertures is placed close to the face plate. .

インライン電子銃は陰極によって3本の電子ビームを共
通平面に発生させ、これらの3電子ビームをフェースプ
レート近辺に集中させるように設計されている。3電子
ビームを集中°させる方法は。
The in-line electron gun is designed to generate three electron beams in a common plane using a cathode and to concentrate these three electron beams near the face plate. 3. How to concentrate the electron beam.

例えば米国特許第2957106号明細書に示されてい
る如く、陰極から射出される電子ビームをはじめから傾
斜している技術があり、又、米国特許第3772554
号明細書に示される如く、電子銃電極に設けられた3電
子ビ一ム通過用開孔のうち一部電極の両側の開孔を電子
銃の中心軸から僅かに外側へ偏位させることにより、電
子ビームの集中を行なっている技術があり、いずれも広
く採用されている。
For example, as shown in US Pat. No. 2,957,106, there is a technique in which the electron beam emitted from the cathode is tilted from the beginning, and US Pat. No. 3,772,554
As shown in the specification, by slightly deviating some of the holes on both sides of the electron beam out of the three electron beam passage holes provided in the electron gun electrode slightly outward from the central axis of the electron gun. There are technologies for concentrating electron beams, both of which are widely used.

カラー受像管の画面(蛍光面)にテレビ画像を表示する
ためには、電子銃から射出した電子ビームを蛍光面全面
に走査するための偏向装置が必要となり、これはファン
ネルのコーン部の外側に取付けられる。偏向装置は基本
的には電子ビームを水平方向に偏向する水平偏向磁界を
発生するための水平偏向コイルおよび電子ビームを垂直
方向に偏向する垂直偏向磁界を発生するための垂直偏向
コイルとを有している。実際のカラー受像管装置におい
ては電子ビームを偏向したときに、3電子ビームスポツ
トのフェースプレートでの集中がくずれてくるので、こ
の集中のくずれを防止するため工夫が施されている。こ
れはコンバーゼンスフリーシステムと称され、水平偏向
磁界をピンクッション形垂直偏向磁界をバレル形にする
ことにより、蛍光面全域に於いて、3電子ビームが集中
するようにしたものである。その結果このシステムでは
コンバーゼンス補正用のパラボラ電流発生回路及びコン
バーゼンス補正磁界を発生させるコンバーゼンスヨーク
が不要になり、コスト低下、生産性向上等多くの効果が
生ずる。
In order to display a television image on the screen (phosphor screen) of a color picture tube, a deflection device is required to scan the electron beam emitted from the electron gun over the entire surface of the phosphor screen. Installed. The deflection device basically includes a horizontal deflection coil for generating a horizontal deflection magnetic field that deflects the electron beam in the horizontal direction and a vertical deflection coil for generating a vertical deflection magnetic field that deflects the electron beam in the vertical direction. ing. In an actual color picture tube device, when the electron beams are deflected, the concentration of the three electron beam spots on the face plate breaks down, so measures are taken to prevent this break in concentration. This is called a convergence free system, and the horizontal deflection magnetic field is made into a pincushion shape, and the vertical deflection magnetic field is made into a barrel shape, so that three electron beams are concentrated over the entire area of the phosphor screen. As a result, this system eliminates the need for a parabolic current generating circuit for convergence correction and a convergence yoke for generating a convergence correction magnetic field, resulting in many effects such as cost reduction and productivity improvement.

〔背景技術の問題点〕[Problems with background technology]

以上述べた如く、カラーブラウン管は多くの開発技術の
採用により品位は向上しているが、管の大形化が普及す
るにつれて新たな問題がクローズアップされつつある。
As mentioned above, the quality of color cathode ray tubes has been improved through the adoption of many developed technologies, but new problems are coming to the fore as the size of tubes becomes more widespread.

すなわち、3電子銃より射出され、フェースプレート上
で集中したビームスポットは、偏向作用を受けない画面
中心では円状のコアのみを提するが、偏向作用を向けた
画面周縁部では偏平化したコアと、上下に広がったフレ
アを提する。その結果画面周縁部では電子ビームのサイ
ズが増大し、フォーカス性能および解像度の劣化が生ず
る。
In other words, the beam spot emitted from the three electron guns and concentrated on the face plate presents only a circular core at the center of the screen where it is not subjected to deflection, but it forms a flattened core at the periphery of the screen where deflection is directed. and a flare that spreads upward and downward. As a result, the size of the electron beam increases at the periphery of the screen, causing deterioration in focus performance and resolution.

〔発、明の目的〕[Purpose of invention]

本発明は以上述べた従来の欠点を解消するためになされ
たもので、画面周縁部における電子ビームスポットの歪
を少なくした画面全域にわたって明るい高解像度が得ら
れるカラー受像装置を提供することを目的とする。
The present invention has been made in order to eliminate the above-mentioned conventional drawbacks, and an object of the present invention is to provide a color image receiving device that can obtain bright high resolution over the entire screen area with less distortion of the electron beam spot at the periphery of the screen. do.

〔発明の概要〕[Summary of the invention]

本発明は3電子銃を水平方向にインライン状に内装した
ネックと、このネックにファンネルを介して接続され内
面に前記電子銃から射出される電子ビームの射突により
赤、緑、青3色に発光する蛍光体層が規則的に被着形成
された蛍光面を有するフェースプレートと、 前記フェースプレートに近接配置され前記電子ビームを
選択的に前記蛍光体層に射突させる多数の開孔を有する
シャドウマスクと、前記ファンネル外壁に装着され前記
電子銃から射出される電子ビームを水平方向に偏向する
水平偏向磁界および垂直方向に偏向する垂直偏向磁界を
発生する偏向装置とを有するカラー受像管装置において
、前記電子銃から射出される3電子ビームは相互にほぼ
平行であり、 前記水平偏向磁界はほぼ斉一磁界分布を形成し、る。
The present invention has a neck in which three electron guns are installed horizontally in line, and the neck is connected to the neck through a funnel, and the inner surface of the neck is illuminated with three colors of red, green, and blue by the impact of the electron beams emitted from the electron guns. a face plate having a phosphor screen on which a light-emitting phosphor layer is regularly deposited; and a large number of apertures arranged close to the face plate to allow the electron beam to selectively impinge on the phosphor layer. In a color picture tube device having a shadow mask and a deflection device attached to the outer wall of the funnel and generating a horizontal deflection magnetic field that deflects the electron beam emitted from the electron gun in the horizontal direction and a vertical deflection magnetic field that deflects the electron beam in the vertical direction. , the three electron beams emitted from the electron gun are substantially parallel to each other, and the horizontal deflection magnetic field forms a substantially uniform magnetic field distribution.

〔発明の実施例〕[Embodiments of the invention]

以下に本発明を実施例に基づいて説明する。第1図は本
発明の20インチ90度偏向のカラー受像管装置の概略
断面図である。
The present invention will be explained below based on examples. FIG. 1 is a schematic cross-sectional view of a 20 inch 90 degree deflection color picture tube device of the present invention.

■はフェースプレート、■はファンネル、(イ)はネッ
クで、いずれもガラス製である。フェースプレート■内
面には赤(R)、緑CG)、青(B)各色に発光する蛍
光体ドツト又は蛍光体ストライプが規則的に配列され映
像表示用の蛍光面■を形成する。
■ is the face plate, ■ is the funnel, and (a) is the neck, all of which are made of glass. On the inner surface of the face plate (2), phosphor dots or stripes that emit light in red (R), green (CG), and blue (B) are regularly arranged to form a fluorescent screen (2) for displaying images.

該蛍光面■に近接対向してシャドウマスク0が配設され
る。シャドウマスク■は通常フェースプレートの内面形
状に相似なドーム状形状をした薄い鉄板からなり、蛍光
面■と対向した部分には電子ビームが正しく蛍光体に射
突するようにあけられた多数の開孔を有している。
A shadow mask 0 is arranged close to and opposite to the phosphor screen (2). The shadow mask ■ usually consists of a thin steel plate with a dome shape similar to the inner surface of the face plate, and the part facing the phosphor screen ■ has many openings so that the electron beams can hit the phosphor correctly. It has holes.

ネックに)内部には赤、緑、青3色に対応する3電子銃
■が封入されている。この3電子銃は水平方向にインラ
イン状に配列され射出する電子ビームが相互に約6.6
■の間隔をもって平行になるように構成されている。各
電子銃は電子ビーム発生源のカソード制御電極、しゃ閉
電極、集束電極。
Inside the neck) are 3 electron guns corresponding to 3 colors: red, green, and blue. These three electron guns are arranged in-line in the horizontal direction, and the emitted electron beams are approximately 6.6
They are constructed so that they are parallel to each other with an interval of (2). Each electron gun has a cathode control electrode, a blocking electrode, and a focusing electrode for the electron beam generation source.

高圧電極から構成され、各々所定の電圧が印加される。It is composed of high-voltage electrodes, each of which is applied with a predetermined voltage.

高圧電極電圧は通常Z5kvの超高電圧でありカラー管
内部が25kvの等電圧に保持される。
The high voltage electrode voltage is normally an ultra-high voltage of Z5 kV, and the inside of the collar tube is maintained at an equal voltage of 25 kV.

ファンネル■のネック(至)接続部近傍はコーン部■と
呼ばれ通常この部分に偏向装置■が装着される。
The area near the neck connection part of the funnel ■ is called the cone part ■, and the deflection device ■ is usually attached to this part.

偏向装置は電子ビームを水平方向に偏向する磁界を発生
する水平偏向磁界と、電子ビームを垂直に偏向する磁界
を発生する垂直偏向磁界よりなる。
The deflection device includes a horizontal deflection magnetic field that generates a magnetic field that deflects the electron beam horizontally, and a vertical deflection magnetic field that generates a magnetic field that deflects the electron beam vertically.

水平偏向磁界について説明する。第2図は本発明の水平
偏向コイルの磁界形状を示す。
The horizontal deflection magnetic field will be explained. FIG. 2 shows the magnetic field shape of the horizontal deflection coil of the present invention.

第3図は画面周縁部におけるビームスポットの形状を示
すもので、(a)は本発明のビームスポット形状、(b
)はピンクッション形磁界形状を用いた従来のビームス
ポット形状である。
FIG. 3 shows the shape of the beam spot at the periphery of the screen, where (a) shows the beam spot shape of the present invention, and (b)
) is a conventional beam spot shape using a pincushion magnetic field shape.

本発明においては第2v1の如く斉一磁界のため。In the present invention, it is due to a uniform magnetic field like 2v1.

水平偏向された電子ビームスポットの形状は大きく改善
される。
The shape of the horizontally deflected electron beam spot is greatly improved.

次に垂直偏向磁界について説明する。第4図は本発明で
採用する上下非対称な偏向磁界形状の例で、(a)は電
子ビームを上方向に偏向する場合の様子を、(b)は下
方向に偏向する場合の様子を表わす、第5図は偏向ヨー
クの上下のトロイダル巻きコイルに付勢する電流のバラ
ンスを偏向方向と偏向量とを対応させて示したものであ
る。実際は下側に配置したコイルに付勢する電流を、破
線は上側に配置したコイルに付勢する電流を示す。
Next, the vertical deflection magnetic field will be explained. Figure 4 shows an example of the vertically asymmetrical deflection magnetic field shape employed in the present invention, with (a) showing the situation when the electron beam is deflected upward, and (b) showing the situation when deflecting it downward. , and FIG. 5 shows the balance of currents energizing the toroidal coils above and below the deflection yoke, with the deflection direction and deflection amount corresponding to each other. Actually, the broken line shows the current that energizes the coil placed on the lower side, and the broken line shows the current that energizes the coil placed on the upper side.

この非対称偏向磁界は偏向磁界の強度の増大とともに磁
界対称軸と電子ビーム軸の間隔りが増大する。すなわち
本発明の構成では両サイド電子ビームは非対称磁界の強
度に比例して外方向の力を受け、垂直軸端に偏向された
場合の電子ビーム間隔を広げる作用を与える。非対称磁
界の強度を適切に選ぶことにより、垂直軸端のビーム間
隔を画面中央の間隔と同一にすることができる。
In this asymmetrical deflection magnetic field, as the intensity of the deflection magnetic field increases, the distance between the magnetic field symmetry axis and the electron beam axis increases. That is, in the configuration of the present invention, the electron beams on both sides receive an outward force in proportion to the strength of the asymmetric magnetic field, which has the effect of widening the distance between the electron beams when deflected to the vertical axis end. By appropriately choosing the strength of the asymmetrical magnetic field, the beam spacing at the vertical axis end can be made the same as the spacing at the center of the screen.

この非対称磁界は電子ビームスポットの偏向歪を最小に
抑制可能である。即ち第4図に示す非対称磁界ではかか
る磁界の強度に比例して両サイドビーム間隔の補正強度
が決まる。言いかえればビーム間隔補正とその時の各ビ
ームの歪量との関係が比例関係にある。これに対し、従
来の上下対称の垂直偏向磁界では各電子ビームが偏向さ
れない場合又は偏向されてもわずかな場合、ビーム間隔
補正は出来ない。
This asymmetric magnetic field can minimize deflection distortion of the electron beam spot. That is, in the case of the asymmetric magnetic field shown in FIG. 4, the correction strength of the distance between both side beams is determined in proportion to the strength of the magnetic field. In other words, the relationship between beam interval correction and the amount of distortion of each beam at that time is proportional. On the other hand, with the conventional vertically symmetrical vertical deflection magnetic field, if each electron beam is not deflected or if it is only slightly deflected, the beam spacing cannot be corrected.

一方各ビームの歪そのものは図から明らかなように位置
によって磁束密度が異なるから当然大きな歪を生ずるこ
ととなる。
On the other hand, as is clear from the figure, the distortion itself of each beam naturally causes large distortion because the magnetic flux density differs depending on the position.

第6図は本発明の上下非対称付加偏向磁界を用いたカラ
ー受像管の画面上のビーム形状を模式的に示す、第7図
は上記対称偏向磁界を用いた従来のカラー受像管のビー
ム形状を模式的に示す。
FIG. 6 schematically shows the beam shape on the screen of a color picture tube using the vertically asymmetric additional deflection magnetic field of the present invention. FIG. 7 shows the beam shape of a conventional color picture tube using the above-mentioned symmetrical deflection magnetic field. Shown schematically.

第6図かられかるように本発明のカラー受像管では両サ
イドビームはより円形化されビームの傾きも少ない。
As can be seen from FIG. 6, in the color picture tube of the present invention, both side beams are more circular and the beam inclination is less.

この傾向は画面全域にわたってあられれる。This tendency can be seen throughout the entire screen.

以上述べた構成によるカラー受像管では、第8図に示す
如く、赤、緑、青3色ビームは画面全域で水平方向に互
いに一定量Δだけ離間する。このままで画像表示を行う
と赤(R)、緑(G)、青(B)各色の画像は上述のΔ
だけ色ズレを生じてしまう。
In the color picture tube configured as described above, as shown in FIG. 8, the three color beams of red, green, and blue are spaced apart from each other by a certain amount Δ in the horizontal direction over the entire screen. If the image is displayed as is, the red (R), green (G), and blue (B) images will be displayed using the above-mentioned Δ
This will cause a color shift.

この色ズレは電子銃に加える信号に対し所定の遅延を行
えば容易に一致させることが出来る。
This color shift can be easily brought into alignment by adding a predetermined delay to the signal applied to the electron gun.

即ち、従来のカラー受像管では白色表示を行うに際しR
,G、B各電子銃に同時に振込み信号を加えるのに対し
本発明のカラー受像管では、G電子銃には所定時間τだ
け遅延させさらにB電子銃では22だけ遅延させる。こ
の遅延時間ではΔ τ“Co−了マW− で決められる。(第9図) ここでHは画面の横巾、fsは水平偏向周波数であり、
Cはオーバスキャン等で決まる定数である。
In other words, in conventional color picture tubes, when displaying white, R
, G, and B electron guns at the same time, in the color picture tube of the present invention, the G electron gun is delayed by a predetermined time τ, and the B electron gun is further delayed by 22. This delay time is determined by Δ τ "Co-terminal W-" (Fig. 9) where H is the width of the screen, fs is the horizontal deflection frequency,
C is a constant determined by overscan or the like.

〔発明の効果〕〔Effect of the invention〕

本発明は以上の構成、作用により画面全域にわたって電
子ビームスポットの歪を少なくした画面が実現され、明
るい高解像度のカラー受像管装置を得ることができる。
The present invention achieves a screen in which the distortion of the electron beam spot is reduced over the entire screen by the above-described configuration and operation, and a bright, high-resolution color picture tube device can be obtained.

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

第1図は本発明のカラー受像管装置の概略断面図、第2
図は本発明に係る偏向装置の水平偏向磁界の形状を説明
する図、第3図は電子ビームスポットの形状を示す図、
第4図は本発明の垂直偏向磁界の形状を説明する図、第
5図は本発明の垂直偏向コイルに付勢される電流の様子
を説明する図、第6図および第7図は電子ビームスポッ
トの形状を説明する図、第8図は画面における3電子ビ
ームのずれ量Δを説明する図、第9図は3電子ビームに
振込む信号の遅延時間τを説明する図である。 1・・・フェースプレート 2・・・ファンネル3・・
・ネック      5・・・蛍光面6°°°シヤドウ
マスク  7・・・電子銃代理人 弁理士 則 近 憲
 佑(ほか1名)第2図 第3図 (a)      (b) 第4図 第5図
FIG. 1 is a schematic sectional view of a color picture tube device of the present invention, and FIG.
The figure is a diagram explaining the shape of the horizontal deflection magnetic field of the deflection device according to the present invention, FIG. 3 is a diagram showing the shape of the electron beam spot,
FIG. 4 is a diagram explaining the shape of the vertical deflection magnetic field of the present invention, FIG. 5 is a diagram explaining the state of the current energized to the vertical deflection coil of the present invention, and FIGS. 6 and 7 are diagrams explaining the shape of the vertical deflection magnetic field of the present invention. FIG. 8 is a diagram for explaining the shape of the spot, FIG. 8 is a diagram for explaining the shift amount Δ of the three electron beams on the screen, and FIG. 9 is a diagram for explaining the delay time τ of the signal transferred to the three electron beams. 1...Face plate 2...Funnel 3...
・Neck 5... Fluorescent screen 6°°° Shadow mask 7... Electron gun agent Patent attorney Noriyuki Chika (and 1 other person) Figure 2 Figure 3 (a) (b) Figure 4 Figure 5

Claims (1)

【特許請求の範囲】[Claims] (1)3電子銃を水平方向にインライン状に内装したネ
ックと、このネックにファンネルを介して接続され内面
に前記電子銃から射出される電子ビームの射突により赤
、緑、青3色に発光する蛍光体層が規則的に被着形成さ
れた蛍光面を有するフェースプレートと、 前記フェースプレートに近接配置され前記電子ビームを
選択的に前記蛍光体層に射突させる多数の開孔を有する
シャドウマスクと、前記ファンネル外壁に装着され前記
電子銃から射出される電子ビームを水平方向に偏向する
水平偏向磁界および垂直方向に偏向する垂直偏向磁界を
発生する偏向装置とを有するカラー受像管装置において
、前記電子銃から射出される3電子ビームは相互にほぼ
平行であり、 前記水平偏向磁界はほぼ斉一磁界分布を形成し、前記垂
直偏向磁界はカラー受像管軸に関し、上下非対称な偏向
磁界カらなることを特徴とするカラー受像管装置。
(1) A neck with 3 electron guns installed horizontally in-line, connected to this neck via a funnel, and created by the impact of the electron beams emitted from the electron guns on the inner surface, producing 3 colors of red, green, and blue. a face plate having a phosphor screen on which a light-emitting phosphor layer is regularly deposited; and a large number of apertures arranged close to the face plate to allow the electron beam to selectively impinge on the phosphor layer. In a color picture tube device having a shadow mask and a deflection device attached to the outer wall of the funnel and generating a horizontal deflection magnetic field that deflects the electron beam emitted from the electron gun in the horizontal direction and a vertical deflection magnetic field that deflects the electron beam in the vertical direction. , the three electron beams emitted from the electron gun are substantially parallel to each other, the horizontal deflection magnetic field forms a substantially uniform magnetic field distribution, and the vertical deflection magnetic field is formed from a vertically asymmetric deflection magnetic field with respect to the color picture tube axis. A color picture tube device characterized by:
JP60133966A 1985-06-20 1985-06-21 Color picture tube device Expired - Lifetime JP2565863B2 (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP60133966A JP2565863B2 (en) 1985-06-21 1985-06-21 Color picture tube device
KR1019860004958A KR900002905B1 (en) 1985-06-20 1986-06-20 Color cathode ray tube
CN198686104329A CN86104329A (en) 1985-06-21 1986-06-20 Colour display tube dence
EP86108417A EP0207394B1 (en) 1985-06-21 1986-06-20 Color cathode ray tube
DE8686108417T DE3674268D1 (en) 1985-06-21 1986-06-20 COLOR CATHODE JET PIPES.
US07/157,130 US4845401A (en) 1985-06-21 1988-02-10 Color cathode ray tube with deflection means

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60133966A JP2565863B2 (en) 1985-06-21 1985-06-21 Color picture tube device

Publications (2)

Publication Number Publication Date
JPS61292840A true JPS61292840A (en) 1986-12-23
JP2565863B2 JP2565863B2 (en) 1996-12-18

Family

ID=15117244

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60133966A Expired - Lifetime JP2565863B2 (en) 1985-06-20 1985-06-21 Color picture tube device

Country Status (1)

Country Link
JP (1) JP2565863B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4876478A (en) * 1987-03-16 1989-10-24 Kabushiki Kaisha Toshiba Cathode ray tube apparatus with improved deflection unit

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS49126223A (en) * 1973-04-04 1974-12-03
JPS5960851A (en) * 1982-09-30 1984-04-06 Toshiba Corp Color picture tube

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS49126223A (en) * 1973-04-04 1974-12-03
JPS5960851A (en) * 1982-09-30 1984-04-06 Toshiba Corp Color picture tube

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4876478A (en) * 1987-03-16 1989-10-24 Kabushiki Kaisha Toshiba Cathode ray tube apparatus with improved deflection unit

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