JPS62237645A - Electron gun - Google Patents

Electron gun

Info

Publication number
JPS62237645A
JPS62237645A JP61082629A JP8262986A JPS62237645A JP S62237645 A JPS62237645 A JP S62237645A JP 61082629 A JP61082629 A JP 61082629A JP 8262986 A JP8262986 A JP 8262986A JP S62237645 A JPS62237645 A JP S62237645A
Authority
JP
Japan
Prior art keywords
electrode
electrode pieces
electron beam
pieces
quadrupole
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
JP61082629A
Other languages
Japanese (ja)
Inventor
Toshio Nakanishi
中西 寿夫
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP61082629A priority Critical patent/JPS62237645A/en
Priority to DE8787302872T priority patent/DE3775253D1/en
Priority to EP87302872A priority patent/EP0241218B1/en
Priority to KR1019870003185A priority patent/KR900006173B1/en
Publication of JPS62237645A publication Critical patent/JPS62237645A/en
Priority to US07/295,883 priority patent/US4886999A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To make it possible to correct the deflecting aberration efficiently without losing the performance, by making furnishing positions and forms of four electrode pieces composing a quadrupole electrode in a position and form almost axis-symmetrical to the elctron beams. CONSTITUTION:A pair of opposing electrode pieces 6a and 6c, and a pair of opposing electrode pieces 6b and 6d compose a horizontal and vertical electric fields respectively. The crossing angle theta of two diagonal planes l and m which combine the middle points in the four gaps 9 formed between the peripheral sides of the four electrode pieces is made within 90 deg.+ or -5 deg., the crossing line p of the two diagonal planes l and m is made almost on the center line of the space surrounded by the four electrode pieces, and the elctron beams 7 are made to pass on the line p. Therefore, the symmetry of the electric field at the center of the space of the quadrupole electrode 6 is maintained, and the section form of the electron beams 7 is converted only from a circular section to a longish oval section including no other excessive deformation. Therefore, the spot image of the electron beams 7 displayed on the fluorescent screen is almost a regular circle, removing only the deflecting aberration.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は偏向収差を補正する四極レンズを形成する電
極を備えた電子銃に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an electron gun equipped with electrodes forming a quadrupole lens for correcting deflection aberration.

〔従来の技術〕[Conventional technology]

陰極線管において電子ビームが偏向磁界によって変形さ
れる所謂偏向収差はよく知られている。
So-called deflection aberration, in which an electron beam is deformed by a deflection magnetic field in a cathode ray tube, is well known.

偏向磁界が非斉一分布の場合は特に著しく、蛍光面中央
で円形スポットであっても、例えば中央部水平端では水
平方向に横長のだ円になり、解像度を劣化させる。この
問題を解消するため、電子銃の集束電極に印加する集束
電圧に、偏向周波数に同期した双曲線波形電圧を重畳さ
せる方法がある。
This is especially noticeable when the deflection magnetic field has a non-uniform distribution, and even if the spot is circular at the center of the phosphor screen, it becomes a horizontally elongated ellipse at the horizontal edge of the central portion, deteriorating the resolution. To solve this problem, there is a method of superimposing a hyperbolic waveform voltage synchronized with the deflection frequency on the focusing voltage applied to the focusing electrode of the electron gun.

しかし、この方法は集束レンズの焦点距離を調整するが
、偏向収差の解消にはならない。
However, although this method adjusts the focal length of the focusing lens, it does not eliminate deflection aberrations.

また、非点収差特性を有する電子レンズを構成する電極
対の一方の14極端部に、非回転対称電界を形成する電
極を設け、静電的に4子レンズと非点収差とを同時に制
御しようという提案がある(特開昭58−9464号公
報)。しかし、この方法は、7E子レンズと非点収差の
異なった目的を、それぞれ満たすための波形電圧が互(
こ電界形成に干渉し合うため、干渉を補正しあう波形信
号をそれぞれに、偏向周波数に同期させて重畳する必要
があるため、動作回路が複雑になり、さらに、インライ
ン型電子銃の場合には、一段にスタティックコンバーゼ
ンスを、電子レンズ領域で静電的に行っているため、こ
の方法では、集束成極電位の変化によってスタティック
コンバーゼンスがくずれるという問題点がある。
In addition, we will provide an electrode that forms a non-rotationally symmetrical electric field at one 14 extreme end of the electrode pair constituting an electron lens with astigmatism characteristics, and try to electrostatically control the quadruplet lens and astigmatism at the same time. There is a proposal (Japanese Unexamined Patent Publication No. 58-9464). However, in this method, the waveform voltages to satisfy the different purposes of the 7E child lens and astigmatism are mutually exclusive.
Since this interferes with the formation of the electric field, it is necessary to superimpose waveform signals that correct each other in synchronization with the deflection frequency, which makes the operating circuit complicated. Since static convergence is performed electrostatically in the electron lens region, this method has the problem that static convergence is disrupted by changes in the focusing polarization potential.

また、陰極線管の外側に電磁石コイルを配設し、陰極線
管内に配備した磁気素子を通して、偏向収差を補正しよ
うという提案がある(特開昭57−84688号公報)
。しかし、この方法は、電磁石の消費電力が大きく、電
磁石コイル等の費用が高い、偏向磁界との干渉を避ける
ための工夫を要する等の問題点がある。
There is also a proposal to correct deflection aberrations by arranging an electromagnetic coil outside the cathode ray tube and using a magnetic element placed inside the cathode ray tube (Japanese Unexamined Patent Publication No. 57-84688).
. However, this method has problems such as high power consumption of the electromagnet, high cost of electromagnetic coils, etc., and the need to take measures to avoid interference with the deflection magnetic field.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

この発明は上記のような問題点を解消するためになされ
たもので、電子銃の基本機能である加速・集束・集中と
いった性能を損うことなく、偏向収差を静電的に効率よ
く補正することのできる電子銃を得ることを目的とする
ものである。
This invention was made to solve the above-mentioned problems, and it is possible to efficiently correct deflection aberration electrostatically without impairing the performance of acceleration, focusing, and concentration, which are the basic functions of an electron gun. The aim is to obtain an electron gun that can

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る°電子銃は、電子ビームを、両側および
上下から挾む4枚の゛成極片で構成されており、かつ、
偏向磁界に同期した偏向収差を補正する波形の補正用集
束電圧が印加される四極電極を備え、この四極電極を構
成する4枚の電極片の配設位置および形状を、1子ビー
ムからみて、はぼ軸対称の位置・形状に構成したもので
ある。
The electron gun according to the present invention is composed of four polar pieces that sandwich the electron beam from both sides and from above and below, and
It is equipped with a quadrupole electrode to which a waveform correcting focusing voltage for correcting deflection aberrations synchronized with the deflection magnetic field is applied, and the arrangement position and shape of the four electrode pieces constituting the quadrupole electrode are as follows when viewed from a single beam: It is constructed in a position and shape that are axially symmetrical.

〔作用〕[Effect]

偏向収差を補正する集束電圧が印加される四極電極は、
その中心を通る電子ビームに、その電子ビームが後に受
ける偏向収差と逆向きの電気力を加えるので、蛍光面上
の全面にわたって真円に近いスポット形状が得られる。
The quadrupole electrode to which a focusing voltage is applied to correct deflection aberration is
Since an electric force is applied to the electron beam passing through the center in the opposite direction to the deflection aberration that the electron beam will later receive, a nearly perfect circular spot shape can be obtained over the entire surface of the phosphor screen.

この電子ビームに加わる電気力は、4枚の電極片の間に
形成される電界は対称性が良いように構成されており、
かつ、電子ビームは4枚の1極片の中心軸上を通るよう
に構成されているので、蛍光面上のスポット形状の真円
度が損なわれることが少ない。
The electric force applied to this electron beam is constructed so that the electric field formed between the four electrode pieces has good symmetry.
In addition, since the electron beam is configured to pass on the central axes of the four single pole pieces, the roundness of the spot shape on the phosphor screen is less likely to be impaired.

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

以下、この発明の一実施例を図によって説明する。 Hereinafter, one embodiment of the present invention will be described with reference to the drawings.

第1図において、同軸とに配置された陰極(1)、制御
1極(2)、加速電F!1(3)、集束、d極(4)を
構成する前側電極(4a)、と後側電極(4b)、およ
び陽極(5)で、電子銃αQの基本部分を構成している
。(6)は四aN極で、前側電極(4a)と後側電g 
(4b)の間に配設されている。制御4 tM (2)
、加速電極(3)、前側電画(4a)には、電子ビーム
(7)が通過する開口部(2a)* (8a)*(4C
)が設けられており、前側電極(4a)と後側?I!極
(4b)とは、接続線(4d)で接続されて同社位に保
持されている。四極?! h (6)は電子ビーム(7
)を両側および上下から挾む4枚の1に極片(6a)*
 (6b)−(6c)−(6d)で構成されており、水
平“rβ極片(6a)と(6C)、垂直電極片(6b)
と(6d〕がそれぞれ対になっており、補正用集束電圧
電源(8)から、偏向収差を補正するのに必要な波形を
もつ補正用集束電圧が印加され、水平方向と垂直方向の
電界を形成する。なお、この実施例では電極片(6a)
、 (6b)、 (6c)、 (6d)を平板で構成し
たが、円弧状であってもよく、平板に限定されるもので
はない。
In Figure 1, a cathode (1), a control pole (2), and an accelerating electrode F! are arranged coaxially with each other. 1 (3), the front electrode (4a), the rear electrode (4b), and the anode (5), which constitute the focusing and d poles (4), constitute the basic part of the electron gun αQ. (6) is a four-a N pole, with the front electrode (4a) and the back electrode g
(4b). Control 4 tM (2)
, the accelerating electrode (3), and the front electrode (4a) have an opening (2a)*(8a)*(4C) through which the electron beam (7) passes.
) is provided, and the front electrode (4a) and the rear electrode (4a) are provided. I! It is connected to the pole (4b) by a connecting wire (4d) and held at the same position. Four poles? ! h (6) is the electron beam (7
) on both sides and top and bottom of the pole piece (6a) *
It consists of (6b)-(6c)-(6d), horizontal rβ pole pieces (6a) and (6C), and vertical electrode piece (6b).
and (6d) are paired, and a correction focusing voltage having a waveform necessary to correct the deflection aberration is applied from the correction focusing voltage power source (8), and the electric field in the horizontal and vertical directions is In this example, the electrode piece (6a)
, (6b), (6c), and (6d) are constructed of flat plates, but they may be arcuate and are not limited to flat plates.

このようにイシ成された電子銃αQは、陰、IM(1)
から放出された1(l子流は、制御7n := (2)
の開口部(2a)と加速1α極(3)の開口部(8a)
を通る間に流量が調節された電子ビーム(7)となって
集束7ペ画(4)の前側電極(4a)の開口部(4C)
から入り、四極電極(6)、後側電極(4b)を通り、
陽極(5)の境界領域で集束作用を受けて蛍光面(図示
せず)にスポット像を映出する。
The electron gun αQ constructed in this way is yin, IM(1)
The 1(l child flow released from the control 7n := (2)
opening (2a) and opening (8a) of acceleration 1α pole (3)
While passing through the electron beam (7), the flow rate of which is adjusted, is focused through the opening (4C) of the front electrode (4a) of the seven-dimensional image (4).
It enters through the quadrupole electrode (6), the rear electrode (4b),
A spot image is projected on a fluorescent screen (not shown) by a focusing action at the boundary area of the anode (5).

第2図は、四極1極(6)の作用を説明するための図で
、たとえば、垂直電極(6b)と(6d)に、水平電極
(6a)と(6C)より正の1llE位を与えた場合、
入射時に円形断面であった電子ビーム(7)は、四極電
極(6)内を通る間に、静電界によって垂直方向の吸引
力をうけ、たて長のtご円形:新面に変形し、偏向磁界
により、蛍光面上でのスポット形状が横長のだ円形にな
る偏向収差を、偏向前に予め補正する。スポット像を画
面中央に映出するときは、四極電極(6)による′+4
子ビーム(7)の断面形状の補正を施さず、電子ビーム
(7)の偏向量に対応して、蛍光面上で円形のスポット
形状が得られる波形をもつ補正用の集束電圧を印加して
1子ビーム(7)の断面形状を遂次変化させる。四極電
極(6)を構成する4枚の電極片は、第3図に示すよう
に、相対向する電極片(6a)と(6c) 、(6b)
と(6d)が、水平方向と垂直方向の電界を構成し、こ
れら4枚の電極片の各周縁部の間に形成される4つの隙
間(9)の中間点を結ぶ2つの対角面l2mが交叉する
角θが90’±5°の範囲内であって、かつ、対角面1
.mが交わる線pが4枚の電極片で囲まれた空間内のほ
ぼ中心線とにあり、この線p上を、電子ビーム(7)が
通るように構成されている。したがって、四極21E極
(6)の空間内の中心部分の電界分布の対称性が保持さ
れているので、電子ビーム(7)の断面形状は円形断面
からたて長だ円形断面に変化するのみで、他の余計な変
形分を含まない。したがって、蛍光面に映出された電子
ビーム(7)のスポット像は真円に近いものとなり、偏
向収差のみを除去することが出来る。
FIG. 2 is a diagram for explaining the action of a single quadrupole (6). For example, the vertical electrodes (6b) and (6d) are given a 1llE position that is more positive than the horizontal electrodes (6a) and (6C). If
While passing through the quadrupole electrode (6), the electron beam (7), which had a circular cross section at the time of incidence, is subjected to a vertical attraction force by the electrostatic field, and is transformed into a new circular surface with a vertical length of t. The deflection aberration that causes the spot shape on the phosphor screen to become a horizontally elongated oval is corrected in advance by the deflection magnetic field before deflection. When projecting a spot image at the center of the screen, use the quadrupole electrode (6) to
Without correcting the cross-sectional shape of the child beam (7), a focusing voltage for correction having a waveform that allows a circular spot shape to be obtained on the phosphor screen is applied in accordance with the amount of deflection of the electron beam (7). The cross-sectional shape of the single beam (7) is successively changed. As shown in FIG. 3, the four electrode pieces constituting the quadrupole electrode (6) are electrode pieces (6a), (6c), and (6b) facing each other.
and (6d) constitute horizontal and vertical electric fields, and two diagonal surfaces l2m connect the midpoints of the four gaps (9) formed between the peripheral edges of these four electrode pieces. The angle θ at which they intersect is within the range of 90'±5°, and the diagonal surface 1
.. A line p where m intersects with the center line of the space surrounded by the four electrode pieces, and the electron beam (7) is configured to pass on this line p. Therefore, since the symmetry of the electric field distribution in the central part of the space of the quadrupole 21E pole (6) is maintained, the cross-sectional shape of the electron beam (7) only changes from a circular cross-section to a vertically oval cross-section. , does not include other unnecessary transformations. Therefore, the spot image of the electron beam (7) projected on the fluorescent screen becomes nearly a perfect circle, and only the deflection aberration can be removed.

なお、1肥実施例では、軸線上に、前後に2分されてい
る集束1極(4)の間に四極電極を配設した例を示した
が、この位置に限られるものではない。
In addition, although the example in which the quadrupole electrode is disposed on the axis between the focusing poles (4) divided into front and rear halves, is not limited to this position.

〔発明の効果〕〔Effect of the invention〕

この発明は以1説明したとおり、電子ビームからみて、
はぼ軸対称形であって、はぼ軸対称の位置に配設されて
いる4枚の電極片でもって構成されており、かつ、偏向
磁界に同期した偏向収差を補正する波形をもつ集束電圧
が印加される四(fi 7?E極を備えた電子銃である
から、電子銃の本質的な集束あるいは集中といった機能
を乱すことがなく、インライン型“i電子銃においても
スタティックコンバーゼンスがくずれるといった欠点も
なく、偏向収差を補正することが出来る。
As explained in 1 below, this invention, from the perspective of an electron beam,
A focusing voltage that is approximately axially symmetrical, consists of four electrode pieces arranged at approximately axially symmetrical positions, and has a waveform that corrects deflection aberrations in synchronization with the deflection magnetic field. Because it is an electron gun equipped with a 4 (fi 7?) E pole, the electron gun's essential functions such as focusing or concentration are not disturbed, and even in an in-line type electron gun, static convergence is not broken. There are no drawbacks and deflection aberrations can be corrected.

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

第1図はこの発明の一実施例の斜視図、第2図はこの実
施例の要部である四極電極の作用を説明するための一部
拡大斜視図、第3図はこの実施例の四極電極の配置を示
す正面図である。 (4)・・・集束電極、(6)・・・四極電極、(6a
)、 (6c)・・・垂直電極片、(6b)、 (ad
)・・・水平辺、1片、(7)・・・電子ビーム、(9
)・・・隙間、αq・・・・E子銃、l9m・・・対角
面、p・・・対角面が交わる線、0・・・交叉角。 なお、各図中、同一符号は同一部分を示す。
FIG. 1 is a perspective view of an embodiment of the present invention, FIG. 2 is a partially enlarged perspective view for explaining the operation of the quadrupole electrode, which is the main part of this embodiment, and FIG. 3 is a perspective view of the quadrupole electrode of this embodiment. FIG. 3 is a front view showing the arrangement of electrodes. (4)... Focusing electrode, (6)... Quadrupole electrode, (6a
), (6c)...vertical electrode piece, (6b), (ad
)...Horizontal side, 1 piece, (7)...Electron beam, (9
)...gap, αq...E gun, l9m...diagonal plane, p...line where diagonal planes intersect, 0...crossing angle. Note that in each figure, the same reference numerals indicate the same parts.

Claims (1)

【特許請求の範囲】[Claims] (1)陰極から放出された電子を電子ビームに形成して
加速する電極と、この電子ビームを集束する電極とを有
する電子銃において、上記電子ビームを両側および上下
から挟むそれぞれ一対の電極片で構成されており、かつ
、これらの電極片に偏向磁界に同期した偏向収差を補正
する波形をもつ補正用集束電圧が印加される四極電極を
備え、上記4枚の電極片の配設位置および形状を、各電
極片の周縁部の間に形成される4つの隙間の中間点を対
角方向に結ぶ2つの対角面の交叉角が90°±5°の範
囲内であり、かつ、その2つの対角面が交わる線上を上
記電子ビームが通るように構成したことを特徴とする電
子銃。
(1) In an electron gun that has an electrode that forms and accelerates electrons emitted from a cathode into an electron beam, and an electrode that focuses this electron beam, a pair of electrode pieces that sandwich the electron beam from both sides and above and below. and a quadripolar electrode to which a correction focusing voltage having a waveform for correcting deflection aberration synchronized with the deflection magnetic field is applied to these electrode pieces, and the arrangement position and shape of the four electrode pieces are The intersection angle of the two diagonal planes diagonally connecting the midpoints of the four gaps formed between the peripheral edges of each electrode piece is within the range of 90° ± 5°, and An electron gun characterized in that the electron beam is configured to pass on a line where two diagonal planes intersect.
JP61082629A 1986-04-03 1986-04-08 Electron gun Pending JPS62237645A (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP61082629A JPS62237645A (en) 1986-04-08 1986-04-08 Electron gun
DE8787302872T DE3775253D1 (en) 1986-04-03 1987-04-02 CATHODE RAY TUBE.
EP87302872A EP0241218B1 (en) 1986-04-03 1987-04-02 Cathode ray tube apparatus
KR1019870003185A KR900006173B1 (en) 1986-04-03 1987-04-03 Cathode ray tube device
US07/295,883 US4886999A (en) 1986-04-03 1989-01-11 Cathode ray tube apparatus with quadrupole electrode structure

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61082629A JPS62237645A (en) 1986-04-08 1986-04-08 Electron gun

Publications (1)

Publication Number Publication Date
JPS62237645A true JPS62237645A (en) 1987-10-17

Family

ID=13779740

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61082629A Pending JPS62237645A (en) 1986-04-03 1986-04-08 Electron gun

Country Status (1)

Country Link
JP (1) JPS62237645A (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54114175A (en) * 1978-02-27 1979-09-06 Hitachi Ltd Deflecting defocus corection electronic gun
JPS58198832A (en) * 1982-05-14 1983-11-18 Matsushita Electronics Corp Cathode-ray tube device
JPS6139347A (en) * 1984-07-30 1986-02-25 Matsushita Electronics Corp Electromagnetic deflection type cathode-ray tube device
JPS6147040A (en) * 1984-08-10 1986-03-07 Matsushita Electronics Corp Color picture tube

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54114175A (en) * 1978-02-27 1979-09-06 Hitachi Ltd Deflecting defocus corection electronic gun
JPS58198832A (en) * 1982-05-14 1983-11-18 Matsushita Electronics Corp Cathode-ray tube device
JPS6139347A (en) * 1984-07-30 1986-02-25 Matsushita Electronics Corp Electromagnetic deflection type cathode-ray tube device
JPS6147040A (en) * 1984-08-10 1986-03-07 Matsushita Electronics Corp Color picture tube

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