JPH09102288A - Deflector - Google Patents

Deflector

Info

Publication number
JPH09102288A
JPH09102288A JP25975295A JP25975295A JPH09102288A JP H09102288 A JPH09102288 A JP H09102288A JP 25975295 A JP25975295 A JP 25975295A JP 25975295 A JP25975295 A JP 25975295A JP H09102288 A JPH09102288 A JP H09102288A
Authority
JP
Japan
Prior art keywords
deflection
coil
magnetic field
deflecting
horizontal
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
JP25975295A
Other languages
Japanese (ja)
Inventor
Shigeru Tsuchida
茂 土田
Masachika Inoue
雅及 井上
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 JP25975295A priority Critical patent/JPH09102288A/en
Publication of JPH09102288A publication Critical patent/JPH09102288A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To improve the focus property of the peripheries of both sides of a self convergence inline type color picture tube. SOLUTION: This deflector has a saddle-type deflecting coil 21 which generates a pin cushion type deflecting magnetic field for deflecting a plurality of beams arranged in a row passing the same plane in the direction of its deflection. Moreover, outside the crossover at the front end of the deflecting coil are provided at least a pair of additional coils 28, which are constituted by winding coils 30, where currents reverse to the deflecting currents flowing to this deflecting coil, synchronizing with the deflection of a plurality of beams by this deflecting coil, flow, around magnetic cores 31.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】この発明は、同一平面上を通
る一列配置の3電子ビームを放出するインライン型カラ
ー受像管に装着される偏向装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a deflecting device mounted on an in-line type color picture tube which emits three electron beams arranged in a row passing through the same plane.

【0002】[0002]

【従来の技術】一般にカラー受像管は、図3に示すよう
に、パネル1およびこのパネル1に接合された漏斗状の
ファンネル2からなる外囲器を有し、そのパネル1の内
面に、青、緑、赤に発光する3色蛍光体層からなる蛍光
体スクリーン3が形成され、この蛍光体スクリーン3に
対向して、その内側に多数の電子ビーム通過孔の形成さ
れたシャドウマスク4が配置されている。一方、ファン
ネル2のネック5内に、3電子ビーム6B ,6G ,6R
を放出する電子銃7が封止されている。そして、この電
子銃7から放出される3電子ビーム6B ,6G ,6R
を、ファンネル2の径大部8とネック5との境界部近傍
の外側に装着された偏向装置9の水平、垂直偏向コイル
10H ,10V の発生する水平、垂直偏向磁界により偏
向して、上記蛍光体スクリーン3を水平、垂直走査する
ことによりカラー画像を表示する構造に形成されてい
る。
2. Description of the Related Art Generally, as shown in FIG. 3, a color picture tube has an envelope composed of a panel 1 and a funnel-shaped funnel 2 joined to the panel 1. , A phosphor screen 3 composed of a three-color phosphor layer that emits green and red light is formed, and a shadow mask 4 having a large number of electron beam passing holes formed therein is arranged so as to face the phosphor screen 3. Has been done. On the other hand, in the neck 5 of the funnel 2, three electron beams 6B, 6G, 6R
The electron gun 7 which emits is sealed. Then, the three electron beams 6B, 6G, 6R emitted from the electron gun 7
Is deflected by the horizontal and vertical deflection magnetic fields generated by the horizontal and vertical deflection coils 10H and 10V of the deflection device 9 mounted on the outer side in the vicinity of the boundary between the large-diameter portion 8 of the funnel 2 and the neck 5, and The body screen 3 is formed in a structure for displaying a color image by horizontal and vertical scanning.

【0003】このようなカラー受像管において、特に電
子銃7を同一水平面上を通る一列配置の3電子ビーム6
B ,6G ,6R を放出するインライン型電子銃とし、図
4に示すように、この電子銃7から放出される一列配置
の3電子ビーム6B ,6G ,6R を偏向する偏向装置の
水平偏向コイルの発生する水平偏向磁界11H をピンク
ッション形、垂直偏向コイルの発生する垂直偏向磁界1
1V をバレル形として、格別の補正回路を要することな
く、3電子ビーム6B ,6G ,6R を蛍光体スクリーン
上に集中するようにしたセルフコンバーゼンス・インラ
イン型カラー受像管が広く実用化されている。
In such a color picture tube, the electron guns 7 are arranged in a row so as to pass the electron guns 7 on the same horizontal plane.
An in-line type electron gun that emits B, 6G and 6R is provided, and as shown in FIG. 4, a horizontal deflection coil of a deflection device that deflects the three electron beams 6B, 6G and 6R arranged in a row emitted from the electron gun 7 is used. Horizontal deflection magnetic field 11H generated is pincushion type, vertical deflection magnetic field generated by vertical deflection coil 1
A self-convergence in-line type color picture tube in which 1V is a barrel type and three electron beams 6B, 6G, and 6R are concentrated on a phosphor screen without requiring a special correction circuit has been widely put into practical use.

【0004】一般に、そのピンクッション形水平偏向磁
界11H を発生する水平偏向コイルはサドル形、バレル
形垂直偏向磁界11V を発生する垂直偏向コイルはトロ
イダル形に形成されている。
In general, the horizontal deflection coil for generating the pincushion type horizontal deflection magnetic field 11H is formed in a saddle shape, and the vertical deflection coil for generating the barrel type vertical deflection magnetic field 11V is formed in a toroidal shape.

【0005】このようなセルフコンバーゼンス・インラ
イン型カラー受像管において、そのフォーカス特性を決
定する主な要因は、電子銃7を構成する制御電極、加速
電極および集束電極であるが、偏向装置9の発生する非
斉一な水平、垂直偏向磁界11H ,11V も、フォーカ
ス特性に大きく関与する。
In such a self-convergence in-line type color picture tube, the main factors that determine the focus characteristics are the control electrode, the acceleration electrode and the focusing electrode that form the electron gun 7, but the deflection device 9 is generated. The inhomogeneous horizontal and vertical deflection magnetic fields 11H and 11V also greatly contribute to the focus characteristics.

【0006】すなわち、上記偏向装置9の発生する水
平、垂直偏向磁界11H ,11V により電子ビーム6B
,6G ,6R を画面周辺部に偏向する場合、電子ビー
ム6B ,6G ,6R は、その水平、垂直偏向磁界11H
,11V の管軸方向成分の影響を受け、偏向磁界の強
度に応じて垂直方向がオーバーフォーカス状態となり、
画面周辺部のビームスポットの形状は歪む。すなわち、
偏向装置の発生する水平、垂直偏向磁界が斉一磁界によ
り電子ビームを偏向する場合は、図5(a)に示すよう
に、画面上のビームスポット13は、その全面にわたり
ほぼ真円となるが、水平偏向磁界11H をピンクッショ
ン形、垂直偏向磁界11V をバレル形とする非斉一磁界
により偏向すると、同(b)に示すように、画面水平軸
(X軸)端では、上記ピンクッション形水平偏向磁界に
より、電子ビームの上半分を下方に、下半分を上方に押
圧する下記ローレンツ力を受け、13a で示すように水
平方向を長軸とする楕円形状に歪む。また画面垂直軸
(Y軸)端では、電子ビームの右半分を右方に、左半分
を左方に押圧するローレンツ力を受け、水平方向を長軸
とする楕円形状に歪み、画面周辺部のフォーカス特性を
劣化させる原因となる。
That is, the electron beam 6B is generated by the horizontal and vertical deflection magnetic fields 11H and 11V generated by the deflection device 9.
, 6G, 6R are deflected to the peripheral part of the screen, the electron beams 6B, 6G, 6R have their horizontal and vertical deflection magnetic fields 11H.
, 11V due to the axial component of the tube, depending on the strength of the deflection magnetic field, the vertical direction becomes overfocus,
The shape of the beam spot around the screen is distorted. That is,
When the horizontal and vertical deflection magnetic fields generated by the deflecting device deflect the electron beam by the uniform magnetic field, the beam spot 13 on the screen becomes almost a perfect circle as shown in FIG. When the horizontal deflection magnetic field 11H is deflected by a non-uniform magnetic field of pincushion type and the vertical deflection magnetic field 11V is barrel type, the pincushion type horizontal deflection is performed at the screen horizontal axis (X axis) end as shown in FIG. The magnetic field receives the following Lorentz force that presses the upper half of the electron beam downward and the lower half upward, and as shown by 13a, it is distorted into an elliptical shape having the major axis in the horizontal direction. At the screen vertical axis (Y-axis) end, a Lorentz force that presses the right half of the electron beam to the right and the left half to the left is distorted into an elliptical shape with the long axis in the horizontal direction, and This causes deterioration of focus characteristics.

【0007】上記ビームスポット13の形状を歪ませる
ローレンツ力については、つぎのように説明することが
できる。すなわち、電子の電荷をe、水平偏向磁界の磁
束密度B(ベクトル)の水平方向成分をBx 、管軸方向
成分をBz 、電子ビームの速度v(ベクトル)の水平方
向成分をvx 、管軸方向成分をvz とすると、ローレン
ツ力F(ベクトル)は、 F=−e(v×B) で表され、その垂直方向成分Fy は、 Fy =−e(vz Bx −vx Bz ) となり、その管軸方向成分は、evx Bz となり、図6
に示すように、電子ビーム6(6B ,6G ,6R )は、
このローレンツ力(管軸方向成分evx Bz )により、
画面水平軸端では、水平方向を長軸とする楕円形状(実
線)に歪む。
The Lorentz force that distorts the shape of the beam spot 13 can be explained as follows. That is, the charge of electrons is e, the horizontal component of the magnetic flux density B (vector) of the horizontal deflection magnetic field is Bx, the tube axis component is Bz, the horizontal component of the velocity v (vector) of the electron beam is vx, and the tube axis direction is Letting the component be vz, the Lorentz force F (vector) is expressed by F = −e (v × B), and its vertical component Fy is Fy = −e (vz Bx −vx Bz), and its tube axis is The directional component is evx Bz, which is shown in FIG.
As shown in, the electron beam 6 (6B, 6G, 6R) is
By this Lorentz force (tube axis direction component evx Bz),
At the horizontal axis of the screen, the image is distorted into an elliptical shape (solid line) whose horizontal axis is the long axis.

【0008】従来この偏向磁界によるフォーカス特性の
劣化について、垂直偏向磁界11Vによる画面長辺付近
(垂直軸端側)でのフォーカス特性の劣化については、
偏向装置の後端部側(ネック側)にコマ補正コイルを付
加することにより補正している。しかし水平偏向磁界1
1H による画面短辺付近(水平軸端側)でのフォーカス
特性の劣化については、補正手段がなかった。
Regarding the deterioration of the focus characteristic due to the deflection magnetic field, regarding the deterioration of the focus characteristic near the long side of the screen (vertical axis end side) due to the vertical deflection magnetic field 11V,
Correction is performed by adding a coma correction coil to the rear end side (neck side) of the deflecting device. However, the horizontal deflection magnetic field 1
Regarding the deterioration of focus characteristics near the short side of the screen (horizontal axis end side) due to 1H, there was no correction means.

【0009】[0009]

【発明が解決しようとする課題】上記のように、同一水
平面上を通る一列配置の3電子ビームを偏向装置の水平
偏向コイルの発生するピンクッション形水平偏向磁界、
垂直偏向コイルの発生するバレル形垂直偏向磁界により
偏向するセルフコンバーゼンス・インライン型カラー受
像管については、その偏向装置の発生する非斉一な偏向
磁界のために、画面周辺部のフォーカス特性が劣化す
る。このフォーカス特性の劣化のうち、垂直偏向磁界に
よる画面長辺付近のフォーカス特性の劣化については、
従来偏向装置の後端部側にコマ補正コイルを付加するこ
とにより補正している。しかし水平偏向磁界による画面
短辺付近のフォーカス特性の劣化については、従来補正
手段がなく、問題となっている。
As described above, the pincushion type horizontal deflection magnetic field generated by the horizontal deflection coil of the deflection device for arranging three electron beams arranged in a row passing on the same horizontal plane,
Regarding the self-convergence in-line type color picture tube which is deflected by the barrel type vertical deflection magnetic field generated by the vertical deflection coil, the focusing characteristics in the peripheral portion of the screen are deteriorated due to the non-uniform deflection magnetic field generated by the deflection device. Among the deterioration of the focus characteristics, the deterioration of the focus characteristics near the long side of the screen due to the vertical deflection magnetic field is
Conventionally, correction is performed by adding a coma correction coil to the rear end side of the deflection device. However, the deterioration of the focus characteristics near the short side of the screen due to the horizontal deflection magnetic field is a problem because there is no conventional correction means.

【0010】この発明は、上記問題に鑑みてなされたも
のであり、セルフコンバーゼンス・インライン型カラー
受像管の画面周辺部、特に画面短辺付近のフォーカス特
性をコンバーゼンス補正を犠牲にすることなく良好にす
ることを目的とする。
The present invention has been made in view of the above problems, and the focus characteristics of the self-convergence in-line type color picture tube on the peripheral portion of the screen, particularly near the short side of the screen, can be improved without sacrificing the convergence correction. The purpose is to do.

【0011】[0011]

【課題を解決するための手段】同一平面上を通る一列配
置の複数ビームをこの複数ビームの配列方向に偏向する
ピンクッション形偏向磁界を発生するサドル型偏向コイ
ルを有する偏向装置において、その偏向コイルの前端部
の渡り線部の外側にこの偏向コイルによる複数ビームの
偏向に同期してこの偏向コイルに流れる偏向電流とは逆
向きの電流が流れるコイルを磁芯に巻回してなる少なく
とも一対の付加コイルを設けた。
A deflection device having a saddle type deflection coil for generating a pincushion type deflection magnetic field for deflecting a plurality of beams arranged in a line passing through the same plane in the arrangement direction of the plurality of beams, the deflection coil Outside the crossover portion of the front end of the, at least a pair of additional coils are formed by winding a coil in which a current flowing in a direction opposite to the deflection current flowing in the deflection coil in synchronization with the deflection of a plurality of beams by the deflection coil is wound around a magnetic core. A coil is provided.

【0012】[0012]

【発明の実施の形態】以下、図面を参照してこの発明の
実施の形態について説明する。
Embodiments of the present invention will be described below with reference to the drawings.

【0013】図1にその一形態であるセルフコンバーゼ
ンス・インライン型カラー受像管の偏向装置を示す。こ
の偏向装置は、カラー受像管のファンネルの径大部とネ
ックとの境界部近傍の外形に対応してほぼ中空台形状に
形成された合成樹脂からなるセパレータ20と、このセ
パレータ20の内側に配置され、ピンクッション形水平
偏向磁界を発生する上下一対のサドル形水平偏向コイル
21と、磁性体からなる中空台形状のコア22に巻回さ
れて、セパレータ20の外側に配置され、バレル形垂直
偏向磁界を発生する上下一対のトロイダル形垂直偏向コ
イル23とからなる。そのサドル形水平偏向コイル21
は、偏向装置の中心軸方向に伸びる直線部25を挟んで
偏向装置の前端部(カラー受像管の蛍光体スクリーン
側)および後端部(カラー受像管のネック側)に、それ
ぞれ渡り線部26,27(26のみ図示)を有する。
FIG. 1 shows a deflecting device of a self-convergence in-line type color picture tube which is one form thereof. This deflecting device is composed of a separator 20 made of synthetic resin formed in a substantially trapezoidal shape corresponding to the outer shape in the vicinity of the boundary between the large-diameter portion of the color picture tube funnel and the neck, and disposed inside the separator 20. A pair of upper and lower saddle type horizontal deflection coils 21 for generating a pincushion type horizontal deflection magnetic field and a hollow trapezoidal core 22 made of a magnetic material are wound around the separator 20. It is composed of a pair of upper and lower toroidal vertical deflection coils 23 that generate a magnetic field. The saddle type horizontal deflection coil 21
Is a crossover portion 26 at the front end (the phosphor screen side of the color picture tube) and the rear end (the neck side of the color picture tube) of the deflector with a straight line portion 25 extending in the central axis direction of the deflector interposed therebetween. , 27 (only 26 is shown).

【0014】さらにこの偏向装置においては、上記水平
偏向コイル21の前端部側の渡り線部26の外側に、セ
パレータ20を介してその渡り線部26を覆うように上
下対称に複数個(図示例では上下に各3個)の付加コイ
ル28が配置されている。
Further, in this deflecting device, a plurality of vertically symmetrical parts are provided outside the connecting line portion 26 on the front end side of the horizontal deflection coil 21 so as to cover the connecting line portion 26 via the separator 20 (illustrated example). In the above, three additional coils 28 are arranged above and below.

【0015】その各付加コイル28は、フェライトなど
の強磁性体からなる直方体状の磁芯30にコイル31を
巻付けたものであり、コイル31の中心軸が偏向装置の
中心軸と同方向になるように、かつ磁芯30の後端部が
水平偏向コイル21の渡り線部26と直線部25との交
点付近まで覆うように配置されている。そしてその各付
加コイル30のコイル31は、水平偏向コイル21に流
れる電流とは逆向きの電流が流れるように水平偏向コイ
ル21に接続されている。
Each additional coil 28 is formed by winding a coil 31 around a rectangular parallelepiped magnetic core 30 made of a ferromagnetic material such as ferrite, and the central axis of the coil 31 is in the same direction as the central axis of the deflecting device. In addition, the rear end of the magnetic core 30 is arranged so as to cover the vicinity of the intersection of the crossover portion 26 and the straight portion 25 of the horizontal deflection coil 21. The coil 31 of each additional coil 30 is connected to the horizontal deflection coil 21 so that the current flowing in the direction opposite to the current flowing in the horizontal deflection coil 21 flows.

【0016】ところで、上記のようにサドル形水平偏向
コイル21の前端部側の渡り線部26の外側に、この渡
り線部26を覆うように複数個の付加コイル28を配置
すると、主としてサドル形水平偏向コイル21の前端部
側の渡り線部26から発生する漏洩磁界を打消し、従来
その漏洩磁界により電子ビームが垂直方向に押圧される
ために生じた画面周辺部のビームスポットの横長形状を
軽減して、フォーカス特性を向上させることができる。
By the way, if a plurality of additional coils 28 are arranged outside the connecting wire portion 26 on the front end side of the saddle type horizontal deflection coil 21 as described above so as to cover the connecting wire portion 26, the saddle shape is mainly obtained. The leakage magnetic field generated from the crossover line portion 26 on the front end side of the horizontal deflection coil 21 is canceled out, and the oblong shape of the beam spot in the peripheral portion of the screen generated by the conventional electron beam being vertically pressed by the leakage magnetic field is formed. The focus characteristics can be reduced to improve the focus characteristics.

【0017】すなわち、図2に示すように、サドル形水
平偏向コイルに33で示す方向の電流が流れると、その
前端部側の渡り線部から破線で示す漏洩磁界34が発生
するが、その渡り線部を覆うように外側に複数個の付加
コイル28を配置し、その各コイル30に水平偏向コイ
ルに流れる電流とは逆向きの電流が流れるように水平偏
向コイルに接続すると、水平偏向コイルによる3電子ビ
ームの偏向に同期して、付加コイル28のまわりに実線
で示す上記漏洩磁界34とは逆向きの磁界35が発生
し、漏洩磁界34を打消す。したがってこの付加コイル
28のコイル30の巻線数やコイル30を流れる電流を
調整することにより、漏洩磁界34を相殺することがで
き、それにより、漏洩磁界34により電子ビームが垂直
方向に押圧されるために生じた画面周辺部のビームスポ
ットの横長形状を軽減して、画面周辺部のフォーカス特
性を向上させることができる。しかもこの付加コイル2
8の発生する磁界35は、3電子ビームの偏向に影響し
ないように調整することにより3電子ビームのコンバー
ゼンス補正を犠牲にしないようにすることができる。
That is, as shown in FIG. 2, when a current flows in the direction indicated by 33 in the saddle type horizontal deflection coil, a leakage magnetic field 34 indicated by a broken line is generated from the crossover portion on the front end side thereof. By arranging a plurality of additional coils 28 outside so as to cover the line portion and connecting to the horizontal deflection coil so that a current in the direction opposite to the current flowing in the horizontal deflection coil flows through each coil 30, the horizontal deflection coil In synchronism with the deflection of the three electron beams, a magnetic field 35 opposite to the leakage magnetic field 34 shown by the solid line is generated around the additional coil 28 to cancel the leakage magnetic field 34. Therefore, the leakage magnetic field 34 can be canceled by adjusting the number of windings of the coil 30 of the additional coil 28 and the current flowing through the coil 30, whereby the leakage magnetic field 34 presses the electron beam in the vertical direction. It is possible to reduce the horizontally elongated shape of the beam spot in the peripheral portion of the screen, which improves the focus characteristics in the peripheral portion of the screen. Moreover, this additional coil 2
The magnetic field 35 generated by 8 can be adjusted so as not to affect the deflection of the 3-electron beam so that the convergence correction of the 3-electron beam is not sacrificed.

【0018】なお、上記実施の形態では、サドル形水平
偏向コイルの渡り線部の外側に上下対称に各3個の付加
コイルを配置したが、この付加コイルは、上下対称に少
なくとも一対配置すればよく、上下対称に各3個以上の
付加コイルを配置してもよい。
In the above embodiment, the three additional coils are arranged vertically symmetrically outside the crossover portion of the saddle type horizontal deflection coil. However, if at least one pair of these additional coils are vertically symmetrically arranged. Of course, three or more additional coils may be arranged vertically symmetrically.

【0019】また、上記実施の形態では、水平偏向コイ
ルがサドル形、垂直偏向コイルがトロイダル形からなる
セミトロイダル形偏向装置について説明したが、この発
明は、水平、垂直偏向コイルがともにサドル形からなる
サドル/サドル形偏向装置に適用して、同様の効果が得
られる。
Further, in the above embodiment, the semi-toroidal type deflection device in which the horizontal deflection coil is a saddle type and the vertical deflection coil is a toroidal type has been described, but in the present invention, the horizontal and vertical deflection coils are both saddle type. The same effect can be obtained by applying the present invention to a saddle / saddle type deflection device.

【0020】[0020]

【発明の効果】同一平面上を通る一列配置の複数ビーム
をこの複数ビームの配列方向に偏向するピンクッション
形偏向磁界を発生するサドル型偏向コイルを有する偏向
装置において、その偏向コイルの前端部の渡り線部の外
側にこの偏向コイルによる複数ビームの偏向に同期して
この偏向コイルに流れる偏向電流とは逆向きの電流が流
れるコイルを磁芯に巻回してなる少なくとも一対の付加
コイルを設けると、画面周辺部のフォーカス特性を劣化
させるサドル型偏向コイルの前端部の渡り線部から発生
する漏洩磁界を打消する磁界を発生させることができ、
それにより、コンバーゼンス補正を犠牲にすることな
く、複数ビームの配列方向の両側の短辺付近のフォーカ
ス特性を向上させることができる。
In a deflector having a saddle type deflection coil for generating a pincushion type deflection magnetic field for deflecting a plurality of beams arranged in a row passing through the same plane in the arrangement direction of the plurality of beams, the front end portion of the deflection coil is If at least a pair of additional coils are provided outside the connecting wire portion, the coils are wound around a magnetic core in which a current flowing in the direction opposite to the deflection current flowing in the deflection coil is provided in synchronization with the deflection of a plurality of beams by the deflection coil. , It is possible to generate a magnetic field that cancels the leakage magnetic field generated from the crossover part of the front end of the saddle type deflection coil that deteriorates the focus characteristics of the peripheral part of the screen,
As a result, it is possible to improve the focus characteristics near the short sides on both sides in the arrangement direction of the plurality of beams without sacrificing the convergence correction.

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

【図1】図1(a)はこの発明の実施の一形態であるセ
ルフコンバーゼンス・インライン型カラー受像管の偏向
装置の構成を示す正面図、図1(b)はその斜視図であ
る。
FIG. 1 (a) is a front view showing the configuration of a deflector for a self-convergence in-line type color picture tube which is an embodiment of the present invention, and FIG. 1 (b) is a perspective view thereof.

【図2】上記偏向装置の作用を説明するための図であ
る。
FIG. 2 is a diagram for explaining the operation of the deflection device.

【図3】カラー受像管の構成を示す図である。FIG. 3 is a diagram showing a configuration of a color picture tube.

【図4】図4(a)はセルフコンバーゼンス・インライ
ン型カラー受像管の偏向装置の発生する水平偏向磁界を
示す図、図4(b)は垂直偏向磁界を示す図である。
4A is a diagram showing a horizontal deflection magnetic field generated by a deflection device of a self-convergence in-line type color picture tube, and FIG. 4B is a diagram showing a vertical deflection magnetic field.

【図5】図5(a)は斉一磁界により偏向された電子ビ
ームの画面上のビームスポットの形状を示す図、図5
(b)は非斉一磁界により偏向された電子ビームの画面
上のビームスポットの形状を示す図である。
5A is a diagram showing the shape of a beam spot on the screen of an electron beam deflected by a uniform magnetic field; FIG.
FIG. 6B is a diagram showing the shape of a beam spot on the screen of the electron beam deflected by the nonuniform magnetic field.

【図6】図6(a)および(b)はそれぞれ上記非斉一
磁界により偏向された電子ビームの歪を説明するための
図である。
6 (a) and 6 (b) are diagrams for explaining the distortion of an electron beam deflected by the non-uniform magnetic field.

【符号の説明】[Explanation of symbols]

20…セパレータ 21…水平偏向コイル 28…付加コイル 30…コイル 31…磁芯 34…漏洩磁界 35…磁界 20 ... Separator 21 ... Horizontal deflection coil 28 ... Additional coil 30 ... Coil 31 ... Magnetic core 34 ... Leakage magnetic field 35 ... Magnetic field

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 同一平面上を通る一列配置の複数ビーム
を上記複数ビームの配列方向に偏向するピンクッション
形偏向磁界を発生するサドル型偏向コイルと、 上記偏向コイルの前端部の渡り線部の外側上に上記偏向
コイルによる複数ビームの偏向に同期して上記偏向コイ
ルに流れる偏向電流とは逆向きの電流が流れるコイルを
磁芯に巻回してなる少なくとも一対の付加コイルとを有
することを特徴とする偏向装置。
1. A saddle type deflection coil for generating a pincushion type deflection magnetic field for deflecting a plurality of beams arranged in a row passing on the same plane in an arrangement direction of the plurality of beams, and a crossover portion of a front end portion of the deflection coil. On the outer side, at least a pair of additional coils formed by winding a coil around which a current flowing in a direction opposite to the deflection current flowing in the deflection coil in synchronization with the deflection of a plurality of beams by the deflection coil is wound. And a deflection device.
JP25975295A 1995-10-06 1995-10-06 Deflector Pending JPH09102288A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25975295A JPH09102288A (en) 1995-10-06 1995-10-06 Deflector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25975295A JPH09102288A (en) 1995-10-06 1995-10-06 Deflector

Publications (1)

Publication Number Publication Date
JPH09102288A true JPH09102288A (en) 1997-04-15

Family

ID=17338469

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25975295A Pending JPH09102288A (en) 1995-10-06 1995-10-06 Deflector

Country Status (1)

Country Link
JP (1) JPH09102288A (en)

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