JPS6238822B2 - - Google Patents

Info

Publication number
JPS6238822B2
JPS6238822B2 JP1273979A JP1273979A JPS6238822B2 JP S6238822 B2 JPS6238822 B2 JP S6238822B2 JP 1273979 A JP1273979 A JP 1273979A JP 1273979 A JP1273979 A JP 1273979A JP S6238822 B2 JPS6238822 B2 JP S6238822B2
Authority
JP
Japan
Prior art keywords
focusing
electrode
electron lens
crossover
lens means
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.)
Expired
Application number
JP1273979A
Other languages
Japanese (ja)
Other versions
JPS54122085A (en
Inventor
Uiriamu Hooken Kenesu
Janko Bojidaa
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.)
Tektronix Inc
Original Assignee
Tektronix Inc
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 Tektronix Inc filed Critical Tektronix Inc
Publication of JPS54122085A publication Critical patent/JPS54122085A/en
Publication of JPS6238822B2 publication Critical patent/JPS6238822B2/ja
Granted 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
    • H01J29/58Arrangements for focusing or reflecting ray or beam
    • H01J29/62Electrostatic lenses
    • H01J29/622Electrostatic lenses producing fields exhibiting symmetry of revolution
    • H01J29/624Electrostatic lenses producing fields exhibiting symmetry of revolution co-operating with or closely associated to an electron gun
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J31/00Cathode ray tubes; Electron beam tubes
    • H01J31/08Cathode ray tubes; Electron beam tubes having a screen on or from which an image or pattern is formed, picked up, converted, or stored
    • H01J31/10Image or pattern display tubes, i.e. having electrical input and optical output; Flying-spot tubes for scanning purposes

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は陰極線管、特にダイナミツク集束補正
回路を具える陰極線管表示装置に関する。
DETAILED DESCRIPTION OF THE INVENTION FIELD OF INDUSTRIAL APPLICATION The present invention relates to cathode ray tubes, and more particularly to cathode ray tube displays comprising a dynamic focusing correction circuit.

〔従来の技術とその問題点〕[Conventional technology and its problems]

文字や図形を表示する画像表示用の従来の電磁
偏向型陰極線管(以下単にCRTという)は、電
子ビームを集束させる為に単一の電子レンズ手段
を使用している。即ち、入口電極と出口電極電位
が互に等しいユニポテンシヤル型電子レンズ(以
下UPLという)と、入口電極と出口電極の電位
が異なるバイポテンシヤル型電子レンズ(以下
BPLという)である。これらCRT、特に表示ス
クリーン面積が大きい(例えば19インチ)場合に
は、表示スクリーンは比較的平面であつて偏向中
心を基準とする球面からのずれが大きいので、表
示スクリーンの中央部で最適集束状態に調整する
と周辺部の集束状態が不完全、即ち、焦点ボケが
生じる。この問題を解決する為に電子ビームの偏
向信号に応じて集束電極電圧を補正する所謂動的
集束補正技法を採用することが考えられる。
Conventional electromagnetic deflection cathode ray tubes (hereinafter simply referred to as CRTs) for displaying images, such as characters and graphics, use a single electron lens means to focus the electron beam. In other words, there are unipotential electron lenses (hereinafter referred to as UPL) in which the entrance and exit electrode potentials are equal to each other, and bipotential electron lenses (hereinafter referred to as UPL) in which the entrance and exit electrodes have different potentials.
(referred to as BPL). In these CRTs, especially when the display screen area is large (for example, 19 inches), the display screen is relatively flat and there is a large deviation from the spherical surface with the center of deflection as a reference, so the optimal focusing is at the center of the display screen. If adjusted to , the convergence state in the peripheral area will be incomplete, that is, the focus will be out of focus. In order to solve this problem, it is conceivable to adopt a so-called dynamic focusing correction technique in which the focusing electrode voltage is corrected according to the deflection signal of the electron beam.

文字図形情報を表示する為のCRTにあつて
は、表示スクリーン全域にわたり極めて高い解像
度(リゾリユーシヨン)が要求される。この用途
のCRTには一般にBTLを使用しており、その平
均集束電圧は電子ビームがスクリーン中央のとき
約3kV以上の高電圧である。斯るBPLを用いる
CRTに動的集束補正を実施し、スクリーン全域
にわたり電子ビームの適正集束状態を得るには、
この約3kV以上の電圧に更に約500Vの大振幅の
補正電圧を印加する必要がある。この補正電圧が
大振幅である理由は、集束電極の平均電圧が高い
(約3kV以上)為に、その電圧変化に対する集束
位置の変化、即ち感度が低い為である。それ故
に、BPLにこの補正電圧を加える集束増幅器は約
3kV以上の高動作電圧から絶縁する必要があり、
構成が複雑となり、高価であり、更に保守サービ
スが不便である。更に、500V程度の大振幅信号
を増幅する増幅デバイスは入手困難であり、高価
であるのみならず信頼性に欠けるという欠点があ
る。
A CRT for displaying character and graphic information requires extremely high resolution over the entire display screen. CRTs for this purpose generally use BTL, whose average focusing voltage is approximately 3 kV or higher when the electron beam is at the center of the screen. Use such BPL
To perform dynamic focusing correction on the CRT and obtain proper focusing of the electron beam across the entire screen,
It is necessary to further apply a large-amplitude correction voltage of about 500V to this voltage of about 3kV or more. The reason why this correction voltage has a large amplitude is that because the average voltage of the focusing electrode is high (approximately 3 kV or more), the change in the focusing position relative to the voltage change, that is, the sensitivity is low. Therefore, the focusing amplifier that adds this correction voltage to the BPL is approximately
Must be isolated from high operating voltages above 3kV,
The configuration is complicated, expensive, and maintenance services are inconvenient. Furthermore, amplification devices that can amplify large amplitude signals of about 500V are difficult to obtain, and have the drawbacks of not only being expensive but also lacking in reliability.

〔発明の目的〕[Purpose of the invention]

従つて、本発明の目的は電子ビームの焦点をス
クリーン全域にわたり動的に補正する為の低電圧
制御手段を有するCRTを提供することである。
It is therefore an object of the present invention to provide a CRT with low voltage control means for dynamically correcting the focus of the electron beam across the screen.

〔発明の概要〕[Summary of the invention]

本発明のCRTはカソード、制御グリツド及び
第1アノードから成る三極管部により電子ビーム
の第1クロスオーバーを形成すると共に、更に
UPLの第1電子レンズ手段とUPL又はBPLの第
2電子レンズ手段を使用して第2電子レンズ部に
第2クロスオーバーを形成し、更に第1電子レン
ズ手段の中央電極に略基準電位で動作する集束増
幅器の出力を印加して第2クロスオーバーの位置
を管軸方向に移動させ、もつて第2電子レンズ手
段により表示スクリーン全域に適正に集束した電
子ビーム像を形成するものである。
The CRT of the present invention forms a first crossover of the electron beam by a triode section consisting of a cathode, a control grid and a first anode;
A second crossover is formed in the second electron lens section using a first electron lens means of the UPL and a second electron lens means of the UPL or BPL, and the central electrode of the first electron lens means is operated at approximately a reference potential. The output of the focusing amplifier is applied to move the position of the second crossover in the direction of the tube axis, so that an electron beam image properly focused over the entire display screen is formed by the second electron lens means.

〔実施例〕〔Example〕

第1図は本発明によるCRTの一実施例の縦断
面図であり、CRT10はネツク部14及びフア
ネル部16より成るガラス製管球12を有する。
クロツク球12内には更にカソード18、制御グ
リツド20及び第1アノード22より成る三極管
部、管軸に沿つて同軸上に配置された略筒状の入
口電極24、中央(又は集束)電極28及び出口
電極26より成るUPLの第1電子レンズ手段、
UPLの一部である電極26とフアネル部16の
内面に設けた導電層30とより成るBPLの第2電
子レンズ手段、及び螢光スクリーン48を有す
る。更に、CRT10の第2電子レンズ手段に略
対応する管球12の外周には偏向コイル42が固
定されている。
FIG. 1 is a longitudinal cross-sectional view of one embodiment of a CRT according to the present invention, and the CRT 10 has a glass tube 12 comprising a neck portion 14 and a funnel portion 16.
Also within the clock bulb 12 are a triode section consisting of a cathode 18, a control grid 20 and a first anode 22, a generally cylindrical entrance electrode 24 coaxially disposed along the tube axis, a central (or focusing) electrode 28, and a triode section consisting of a cathode 18, a control grid 20 and a first anode 22; first electron lens means of the UPL consisting of an exit electrode 26;
The second electron lens means of the BPL comprises an electrode 26 that is part of the UPL, a conductive layer 30 on the inner surface of the funnel 16, and a fluorescent screen 48. Further, a deflection coil 42 is fixed to the outer periphery of the bulb 12, which substantially corresponds to the second electron lens means of the CRT 10.

カソード18は例えば基準電位又は接地電位と
なし、その内にヒータコイル32を有し、熱電子
を放出する。制御グリツド20はカソード18に
対し負バイアス電圧、例えば−50Vの電源に接続
し、カソード18から放出した電子ビーム36が
通過する開口34を有し、この開口34で電子ビ
ーム36を整形して、その電子密度を決定する。
制御グリツド20は電子ビーム36に作用してそ
れを集束し、第1クロスオーバーC1を制御グリ
ツド20と第1アノード22間に形成する。
The cathode 18 has a reference potential or ground potential, has a heater coil 32 therein, and emits thermoelectrons. The control grid 20 is connected to a power source with a negative bias voltage, for example -50V, with respect to the cathode 18, and has an aperture 34 through which the electron beam 36 emitted from the cathode 18 passes, and shapes the electron beam 36 with the aperture 34. Determine its electron density.
Control grid 20 acts on and focuses electron beam 36 to form a first crossover C 1 between control grid 20 and first anode 22 .

第1アノード22はカソード18に対して正電
位、例えば1kVの電源に接続され、電子ビーム3
6が通過するビーム形成開口38を有する。この
第1アノード22で形成した電界は、電子ビーム
36に作用してUPL手段の入口電極24中を電
子ビームが移動するにつれて発散する。UPL手
段の中央電極24と出口電極26には同一電圧、
例えば2kVを印加する。入口電極24は電子ビー
ム36が通過するビーム形成開口40を有する。
電子ビーム36は、この電極24を通過し、中央
(集束)電極28に近づくにつれて発散する。
The first anode 22 is connected to a power source at a positive potential, for example 1 kV, with respect to the cathode 18, and the electron beam 3
6 has a beam-forming aperture 38 through which it passes. The electric field created by this first anode 22 acts on the electron beam 36 and diverges as it moves through the entrance electrode 24 of the UPL means. The same voltage is applied to the central electrode 24 and the exit electrode 26 of the UPL means,
For example, apply 2kV. Entrance electrode 24 has a beam-forming aperture 40 through which electron beam 36 passes.
The electron beam 36 passes through this electrode 24 and diverges as it approaches the central (focusing) electrode 28 .

従来設計の水平及び垂直偏向コイル42を管球
12の外周に設け、従来のX及びY偏向回路44
により発生した偏向信号により駆動する。偏向回
路44から必要な波形変換を行つて得た集束補正
信号を集束増幅器46に入力し、その増幅出力を
集束電極28に印加する。集束電極28には高電
圧が印加されていないので、集束増幅器46の出
力電圧は例えば0乃至100Vの低電圧且つ低振幅
であり、その電圧レベルは偏向コイル42により
電子ビーム36に与えられる偏向の度合に依存す
ることに注目されたい。即ち、偏向により電子ビ
ーム36が管軸から外れるにつれて集束電極28
の電圧も変化し、これによりUPLの電界を変化
して電子ビーム36の第2クロスオーバーC2
位置をUPLの出口電極26内の異なる管軸上の
位置に移動させる。
Horizontal and vertical deflection coils 42 of conventional design are provided around the outer periphery of bulb 12, and conventional X and Y deflection circuits 44 are provided.
It is driven by the deflection signal generated by. A focusing correction signal obtained by performing necessary waveform conversion from the deflection circuit 44 is input to the focusing amplifier 46, and its amplified output is applied to the focusing electrode 28. Since no high voltage is applied to the focusing electrode 28, the output voltage of the focusing amplifier 46 is a low voltage and low amplitude, for example, 0 to 100 V, and the voltage level is equal to the deflection given to the electron beam 36 by the deflection coil 42. Note that it is degree dependent. That is, as the electron beam 36 deviates from the tube axis due to deflection, the focusing electrode 28
The voltage at is also changed, thereby changing the electric field of the UPL and moving the position of the second crossover C 2 of the electron beam 36 to a different tube axis position within the exit electrode 26 of the UPL.

導電層30は例えば18kVの高圧電源に接続さ
れると共に例えば周知のP4型螢光体で形成した
従来の螢光スクリーン48と係合し、この螢光ス
クリーン48にも18kVが印加されるようにす
る。電子ビーム36の第2クロスオーバーC2
BPLにより螢光スクリーン48のあらゆる表示位
置で正しく焦点を結ぶこととなる。尚、螢光スク
リーン48は異なる発光色の複数の螢光体層を積
層し、高圧電源をスイツチ54で例えば18kVと
12kVで切換えることにより発光色を変える周知
のビームペネトレーシヨン型であつてもよい。発
光色を切換えることにより螢光スクリーン48に
表示される情報の識別力を改善することが可能で
あるので、特に高密度文字又は図形表示装置に好
適である。
The conductive layer 30 is connected to a high voltage power source, for example 18 kV, and engages a conventional fluorescent screen 48 formed of, for example, the well-known P4 type phosphor, such that 18 kV is also applied to the fluorescent screen 48. do. The second crossover C 2 of the electron beam 36 is
BPL ensures proper focus at all display positions on the fluorescent screen 48. Incidentally, the fluorescent screen 48 is made by laminating a plurality of fluorescent layers of different emission colors, and the high voltage power source is set to 18 kV by a switch 54, for example.
It may be a well-known beam penetration type that changes the emission color by switching at 12 kV. It is particularly suitable for high-density character or graphic display devices, as it is possible to improve the discrimination of information displayed on the fluorescent screen 48 by switching the luminescent color.

この実施例のCRT表示装置では、UPLを構成
する集束(中央)電極28の電圧を偏向信号に応
じて変化することにより電子ビーム36の第2ク
ロスオーバーC2の位置を出口電極26内で制御
することにより偏向集束歪を補正している。この
集束歪補正は略基準電位で動作する集束電極28
の電圧を制御して行うので、この動的補正電圧に
よる電子ビーム36の第2クロスオーバーC2
位置の変化は大きい。即ち、高感度であり、必要
とする補正電圧振幅が従来の場合(約500V)に
比して低い(約100V)。その為に、集束増幅器4
6は高電圧型や絶縁型である必要はなく、従来の
素子を使用し簡単且つ安価に構成でき、しかも低
消費電力、高信頼性であり、保守サービスも容易
である。
In the CRT display device of this embodiment, the position of the second crossover C2 of the electron beam 36 is controlled within the exit electrode 26 by changing the voltage of the focusing (center) electrode 28 constituting the UPL in accordance with the deflection signal. By doing so, deflection and focusing distortion is corrected. This focusing distortion correction is performed using a focusing electrode 28 that operates at approximately a reference potential.
Since this is done by controlling the voltage of , the change in the position of the second crossover C 2 of the electron beam 36 due to this dynamic correction voltage is large. That is, it has high sensitivity and the required correction voltage amplitude is lower (approximately 100V) than in the conventional case (approximately 500V). For that purpose, the focusing amplifier 4
6 does not need to be a high voltage type or an insulated type, and can be constructed easily and inexpensively using conventional elements, and has low power consumption, high reliability, and easy maintenance service.

第2図は本発明の他の実施例のCRTであり、
第1図の実施例と同様素子には類似参照符号を付
している。第2図では第2電子レンズ手段として
第1図のBPLに代り、第2UPLを使用している。
第1UPLは入口電極24、中央(集束)電極28
及び出口電極26で構成され、入出口電極24−
26は共に18kVの高圧電源に接続されている。
集束電極28は集束増幅器46の出力側に接続さ
れ、動的集束歪補正のため0−200Vの範囲で変
化する。第2UPLは第1UPLの出口電極26を共
用して入口電極とし、約0Vの中央電極52と出
口電極50とにより構成される。
FIG. 2 shows a CRT according to another embodiment of the present invention.
Elements similar to those of the embodiment of FIG. 1 have been given like reference numerals. In FIG. 2, a second UPL is used as the second electron lens means instead of the BPL in FIG. 1.
The first UPL is the entrance electrode 24, the center (focusing) electrode 28
and an exit electrode 26, and an entrance and exit electrode 24-
26 are both connected to an 18kV high voltage power supply.
The focusing electrode 28 is connected to the output of the focusing amplifier 46 and varies from 0-200V for dynamic focusing distortion correction. The second UPL shares the exit electrode 26 of the first UPL as an entrance electrode, and is composed of a central electrode 52 of about 0V and an exit electrode 50.

第2図の実施例のCRTは基本的に第1図の
CRTと同様であるので、詳細説明は省略する。
ここで、集束増幅器46の出力電圧により、略出
口電極26内に形成される電子ビームの第2クロ
スオーバーが管軸に沿つて移動し、第2UPLによ
り螢光スクリーン48上に正しく像を形成する。
尚、第2図のCRTでも螢光スクリーン48は単
一発光色のものでもよいが、赤、緑、青又はその
他所望の発光色の螢光体を積層した又は各螢光粒
子を多層コーテイングした従来のペネトレーシヨ
ン型螢光体であつてもよい。その場合、スイツチ
手段54で選択的に18kV又は12kVを螢光スクリ
ーン48に印加する。例えば、12kVのときは
赤、18kVのときは緑の発光色の情報表示が得ら
れる。また、螢光スクリーン48の電圧を任意に
選択すると、赤、橙、黄及び緑の間で連続的に変
化する発光色が得られる。また、導電層30の電
圧を切換えると、生じる電界も変化するので、最
適集束状態を得る為に第1UPLの入出口電極24
−26の電圧もスイツチ54で切換えるよう構成
している。
The CRT in the embodiment shown in Figure 2 is basically the same as in Figure 1.
Since it is similar to CRT, detailed explanation will be omitted.
Here, due to the output voltage of the focusing amplifier 46, a second crossover of the electron beam formed approximately in the exit electrode 26 is moved along the tube axis, and is properly imaged on the fluorescent screen 48 by the second UPL. .
In the case of the CRT shown in FIG. 2, the fluorescent screen 48 may have a single luminescent color, but it may also be one in which phosphors of red, green, blue, or other desired luminescent color are laminated or each fluorescent particle is coated in multiple layers. It may be a conventional penetration type phosphor. In that case, switch means 54 selectively applies 18 kV or 12 kV to fluorescent screen 48. For example, information can be displayed in red when the voltage is 12kV and green when the voltage is 18kV. Further, by arbitrarily selecting the voltage of the fluorescent screen 48, a continuously changing emission color is obtained between red, orange, yellow and green. Furthermore, when the voltage of the conductive layer 30 is changed, the generated electric field also changes, so in order to obtain the optimum focusing state, the input and exit electrodes 24 of the first UPL are
-26 voltage is also switched by switch 54.

〔発明の効果〕〔Effect of the invention〕

上述の説明から明らかな如く、本発明のCRT
では従来の大型電磁偏向CRTに一般的に使用さ
れていたBPLに代り、UPLの第1電子レンズ手段
と、BPL又はUPLの第2電子レンズ手段の2個の
電子レンズ手段を採用している。この第1電子レ
ンズ手段により第1及び第2電子レンズ手段の一
部となる電極26内に電子ビームの第2クロスオ
ーバーを生じさせ、これを第2電子レンズ手段に
より螢光スクリーン上に結像させている。略基準
電位で動作する第1電子レンズ手段の中央(集
束)電極を集束増幅器の出力電圧により偏向信号
に応じて制御することにより、第2クロスオーバ
ー位置を管軸にそつて移動させ、これにより螢光
スクリーンの全域にわたり最適集束状態が得られ
る。しかも、集束増幅器は何等絶縁をする必要が
なく、しかもその補正電圧は約100乃至200Vの低
電圧であるので市販の安価な素子を使用し簡単に
実現でき、しかも高信頼性であり、保守サービス
も容易であるという種々の顕著な効果を有する。
As is clear from the above description, the CRT of the present invention
In place of the BPL commonly used in conventional large electromagnetic deflection CRTs, the present invention employs two electron lens means: a first electron lens means of UPL and a second electron lens means of BPL or UPL. The first electron lens means causes a second crossover of the electron beam into the electrode 26 forming part of the first and second electron lens means, which is imaged onto a fluorescent screen by the second electron lens means. I'm letting you do it. The second crossover position is moved along the tube axis by controlling the central (focusing) electrode of the first electron lens means, operating at approximately the reference potential, by the output voltage of the focusing amplifier in response to the deflection signal; Optimal focusing is achieved over the entire area of the fluorescent screen. Moreover, the focusing amplifier does not require any insulation, and its correction voltage is a low voltage of about 100 to 200V, so it can be easily realized using commercially available inexpensive elements, and it is highly reliable and requires no maintenance service. It has various remarkable effects such as being easy to use.

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

第1図は本発明によるCRTの一実施例の縦断
面図、第2図は本発明によるCRTの他の実施例
の縦断面図を示す。 図中、18はカソード、20は制御グリツド、
22は第1アノード、24,26,28は第1電
子レンズ手段、26,30又は26,50,52
は第2電子レンズ手段、42は偏向コイル、44
は偏向回路、46は集束増幅器を示す。
FIG. 1 is a longitudinal cross-sectional view of one embodiment of the CRT according to the present invention, and FIG. 2 is a longitudinal cross-sectional view of another embodiment of the CRT according to the present invention. In the figure, 18 is a cathode, 20 is a control grid,
22 is a first anode; 24, 26, 28 are first electron lens means; 26, 30 or 26, 50, 52
42 is a second electron lens means; 42 is a deflection coil; 44 is a deflection coil;
indicates a deflection circuit, and 46 indicates a focusing amplifier.

Claims (1)

【特許請求の範囲】 1 電子ビームを放射するカソードと、該カソー
ド近傍に位置し該カソードに対し負電位が印加さ
れる制御グリツドと、該制御グリツド近傍に位置
し上記カソードに対し正電位が印加される第1ア
ノードとを有し、該第1アノード及び上記制御グ
リツドの電位により上記制御グリツドと第1アノ
ード間に第1クロスオーバーを生じる陰極線管に
おいて、 電子ビーム路に沿つて順次同軸状に配置された
略円筒状の入口、中央及び出口電極を有し、該出
口電極部内の異なる管軸方向位置に第2クロスオ
ーバーを生じる十分な強度の電界を形成するユニ
ポテンシヤル形の第1電子レンズ手段と、該第1
電子レンズ手段の上記出口電極を一部に含む第2
電子レンズ手段と、該第2電子レンズ手段により
上記第2クロスオーバーからの電子ビームが集束
される表示スクリーンと、陰極線管の偏向信号に
応じて比較的低電圧の可変集束補正電圧を発生し
上記第1電子レンズ手段の上記中央電極に印加し
て上記第2クロスオーバー位置を変化させ偏向歪
を補正する集束増幅器とを具えることを特徴とす
る陰極線管。
[Scope of Claims] 1. A cathode that emits an electron beam, a control grid located near the cathode to which a negative potential is applied, and a control grid located near the control grid to which a positive potential is applied to the cathode. a first anode, the potential of the first anode and the control grid creating a first crossover between the control grid and the first anode; a unipotential first electron lens having generally cylindrical entrance, center and exit electrodes arranged to form an electric field of sufficient strength to cause a second crossover at different tube axial positions within the exit electrode section; means and said first
a second part of which the exit electrode of the electron lens means is included;
electron lens means; a display screen on which the electron beam from the second crossover is focused by the second electron lens means; A cathode ray tube comprising: a focusing amplifier for applying voltage to the central electrode of the first electron lens means to change the second crossover position and correct deflection distortion.
JP1273979A 1978-02-15 1979-02-06 Cathode ray tube Granted JPS54122085A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US87804278A 1978-02-15 1978-02-15

Publications (2)

Publication Number Publication Date
JPS54122085A JPS54122085A (en) 1979-09-21
JPS6238822B2 true JPS6238822B2 (en) 1987-08-19

Family

ID=25371251

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1273979A Granted JPS54122085A (en) 1978-02-15 1979-02-06 Cathode ray tube

Country Status (6)

Country Link
JP (1) JPS54122085A (en)
CA (1) CA1132649A (en)
DE (1) DE2905479C2 (en)
FR (1) FR2417850A1 (en)
GB (1) GB2015195A (en)
NL (1) NL7901041A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4277722A (en) * 1978-02-15 1981-07-07 Tektronix, Inc. Cathode ray tube having low voltage focus and dynamic correction
JPH0719541B2 (en) * 1985-04-30 1995-03-06 株式会社日立製作所 In-line color picture tube

Family Cites Families (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
BE430157A (en) *
GB495707A (en) * 1937-04-17 1938-11-17 Frederick Hermes Nicoll Improvements in or relating to focussing systems for use in electric discharge tubes
US2252441A (en) * 1937-04-26 1941-08-12 Loewe Opta Gmbh Sharp-edge deflection
GB505751A (en) * 1937-09-13 1939-05-15 Frederick Hermes Nicoll Improvements in or relating to cathode ray tubes
US3023336A (en) * 1957-10-25 1962-02-27 Tektronix Inc Cathode ray tube having post acceleration
NL253491A (en) * 1959-07-07
DE1439720B2 (en) * 1964-08-27 1976-04-08 Telefunken Patentverwertungsgesellschaft Mbh, 7900 Ulm CATHODE TUBE WITH DEFLECTORS
JPS4811664B1 (en) * 1965-04-26 1973-04-14
GB1204314A (en) * 1966-09-21 1970-09-03 Atomic Energy Authority Uk Improvements in or relating to nuclear reactors
US3622836A (en) * 1968-03-25 1971-11-23 Eastman Kodak Co Deflection amplifier with dynamic focus control
JPS5743972B1 (en) * 1971-02-05 1982-09-18
BE785749A (en) * 1971-07-02 1973-01-02 Philips Nv TELEVISION CAMERA TUBE (VIDICON) IN WHICH THE ADVERSE INFLUENCE OF THE RETURN BEAM IS COUNTERLED
FR2166165B1 (en) * 1971-12-30 1976-10-29 Hitachi Ltd
JPS5543660Y2 (en) * 1972-04-12 1980-10-14
FR2201536B1 (en) * 1972-09-26 1976-08-13 Thomson Csf

Also Published As

Publication number Publication date
DE2905479C2 (en) 1984-12-13
FR2417850B1 (en) 1981-10-09
NL7901041A (en) 1979-08-17
JPS54122085A (en) 1979-09-21
FR2417850A1 (en) 1979-09-14
DE2905479A1 (en) 1979-08-16
GB2015195A (en) 1979-09-05
CA1132649A (en) 1982-09-28

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