JPS6138574B2 - - Google Patents

Info

Publication number
JPS6138574B2
JPS6138574B2 JP52152422A JP15242277A JPS6138574B2 JP S6138574 B2 JPS6138574 B2 JP S6138574B2 JP 52152422 A JP52152422 A JP 52152422A JP 15242277 A JP15242277 A JP 15242277A JP S6138574 B2 JPS6138574 B2 JP S6138574B2
Authority
JP
Japan
Prior art keywords
permanent magnet
ray tube
magnetic field
focusing
electron gun
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
JP52152422A
Other languages
Japanese (ja)
Other versions
JPS5484966A (en
Inventor
Soichi Sakurai
Kyohei Fukuda
Masanobu Takada
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP15242277A priority Critical patent/JPS5484966A/en
Publication of JPS5484966A publication Critical patent/JPS5484966A/en
Publication of JPS6138574B2 publication Critical patent/JPS6138574B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明は陰極線管電子銃に関するものであり、
特に小型、軽量でかつフオーカス調整も容易な電
磁界集束方式陰極線管電子銃に関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a cathode ray tube electron gun,
In particular, the present invention relates to an electromagnetic field focusing type cathode ray tube electron gun that is small, lightweight, and easy to focus.

第1図は従来の磁界集束方式の陰磁線管電子銃
の概略図である。ヒータ2によつて加熱されるカ
ソード電極3から飛び出した電子は第1グリツド
電極4、第2グリツド電極5によつて形成される
三極レンズおよびプリフオーカスレンズによつて
集束作用を受け、いわゆるクロスオーバを形成す
る。その後、第3グリツド電極6によつて電子は
一定の発散角をもつて加速され、第3グリツド電
極6のほゞ中央部に位置し、真空外囲器1の外に
装着された電磁集束コイル7aによつて作られる
磁界レンズで集束され、クロスオーバはけい光面
上(図示せず)に写し出される。この場合、電磁
集束コイル7aに流れる電流を増減し、磁界レン
ズの強さを適当な値に設定する事によつてクロス
オーバがけい光面でジヤストフオーカスするよう
にしていた。なお、9は内部導電膜10と第3グ
リツド電極6を導電接続するコンタクトスプリン
グである。しかしながら電磁集束コイル7aのみ
によつて集束に必要な磁界を発生させようとする
と、コイルの重量、体積が共に大きくなつて、コ
スト的にも高いものとなるので、ごく限られた高
解像度が厳しく要求される製品のみにしか磁界集
束方式は適用されてないのが現状である。しかも
電磁集束コイル7aを具備した場合は、コイル電
流による発熱等によつて集束磁界の強さが著しく
変動するため、温度補正用回路を必要とし回路側
のコストも上昇してしまう欠点もあつた。
FIG. 1 is a schematic diagram of a conventional magnetic field focusing type negative magnetic ray tube electron gun. Electrons emitted from the cathode electrode 3 heated by the heater 2 are focused by a triode lens and a prefocus lens formed by the first grid electrode 4 and the second grid electrode 5, and are thus form a crossover. Thereafter, the electrons are accelerated by the third grid electrode 6 at a constant divergence angle, and the electromagnetic focusing coil is located approximately in the center of the third grid electrode 6 and is attached to the outside of the vacuum envelope 1. 7a, and the crossover is imaged onto a fluorescent surface (not shown). In this case, the crossover is just focused on the fluorescent surface by increasing or decreasing the current flowing through the electromagnetic focusing coil 7a and setting the strength of the magnetic field lens to an appropriate value. Note that 9 is a contact spring that conductively connects the internal conductive film 10 and the third grid electrode 6. However, if an attempt is made to generate the magnetic field necessary for focusing using only the electromagnetic focusing coil 7a, the weight and volume of the coil will increase, and the cost will also be high. At present, the magnetic field focusing method is only applied to products that require it. Moreover, when the electromagnetic focusing coil 7a is provided, the strength of the focusing magnetic field fluctuates significantly due to heat generated by the coil current, etc., so a temperature correction circuit is required, which increases the cost of the circuit. .

そこで本発明の目的は、上記した従来技術の欠
点をなくし、集束装置の重量、体積が共に小さ
く、コストも低く、さらにフオーカス調整が容易
に行なえる電磁界集束方式の新規な陰極線管を提
供するにある。
SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a new cathode ray tube using an electromagnetic field focusing method, which eliminates the above-mentioned drawbacks of the prior art, has a focusing device that is small in weight and volume, is low in cost, and allows easy focus adjustment. It is in.

本発明は集束用磁界の発生手段として導電性の
永久磁石を使用し、該永久磁石を真空外囲器に内
蔵し、所望に応じ該永久磁石にフオーカス調整用
電圧を加えて、上記目的を達成しようとするもの
である。
The present invention achieves the above object by using a conductive permanent magnet as a means for generating a focusing magnetic field, incorporating the permanent magnet in a vacuum envelope, and applying a focus adjustment voltage to the permanent magnet as desired. This is what I am trying to do.

以下本発明の実施例を詳細に説明する。 Examples of the present invention will be described in detail below.

第2図は本発明の1実施例の断面図であり、第
1図と同一の符号は同一部分をあらわす。7bは
例えばアルニコ系磁石等の導電性材料で作られた
円筒形永久磁石、8は第4グリツド電極である。
図において第2グリツド電極5の開口部付近に形
成された電子のクロスオーバは一定の発散角をも
つて第3グリツド電極6で加速された後、永久磁
石7bによつて形成される磁界レンズで集束さ
れ、けい光面の近傍に焦点をむすぶ。その際前記
永久磁石7bに外部から適当な電圧E2を加える
ことにより、永久磁石7bの前後の、第3グリツ
ド電極6および第4グリツド電極8との間の間隙
部には1対の電界レンズが形成され、これら3つ
のレンズの複合収束作用によつて電子が完全にけ
い光面上に焦点を結ぶようにすることが出来る。
例えば20インチ110゜偏向の陰極線管において陽
極電圧E1=5.0KV、永久磁石の軸上集束磁場が
400ガウスの場合、永久磁石7bに加える電圧を
4.3KV前後にした時丁度けい光面上に焦点を結ば
せることができた。
FIG. 2 is a sectional view of one embodiment of the present invention, and the same reference numerals as in FIG. 1 represent the same parts. 7b is a cylindrical permanent magnet made of a conductive material such as an alnico magnet, and 8 is a fourth grid electrode.
In the figure, the electron crossover formed near the opening of the second grid electrode 5 is accelerated by the third grid electrode 6 with a certain divergence angle, and then is formed by a magnetic field lens formed by the permanent magnet 7b. It is focused and focuses near the fluorescent surface. At this time, by applying an appropriate voltage E2 to the permanent magnet 7b from the outside, a pair of electric field lenses are installed in the gap between the third grid electrode 6 and the fourth grid electrode 8 before and after the permanent magnet 7b. is formed, and the combined focusing action of these three lenses allows the electrons to be completely focused on the phosphorescent surface.
For example, in a 20-inch 110° deflection cathode ray tube, the anode voltage E 1 = 5.0 KV and the axial focusing magnetic field of the permanent magnet.
In the case of 400 Gauss, the voltage applied to permanent magnet 7b is
When I set the voltage to around 4.3KV, I was able to focus exactly on the fluorescent surface.

以上においては、1個の導電性円筒形永久磁石
を電子銃電極系の中に用いた例を示したが、複数
の永久磁石を用いてもよく、また特定のグリツド
電極の一部のみを永久磁石で置換した構造として
もよいことは明らかである。第3図は後者の1例
を示し、第3グリツド6の一部がそれと同一内径
の導電性円筒形永久磁石7cで置換されたものと
みることができ、その動作は第2図の場合と同様
である。
In the above example, one conductive cylindrical permanent magnet is used in the electron gun electrode system, but multiple permanent magnets may be used, or only a part of a particular grid electrode is used as a permanent magnet. It is clear that a structure in which magnets are substituted may also be used. FIG. 3 shows an example of the latter, in which a part of the third grid 6 can be seen as being replaced by a conductive cylindrical permanent magnet 7c having the same inner diameter as that of the third grid 6, and its operation is similar to that in FIG. The same is true.

以上述べたように本発明では真空外囲器内に導
電性の永久磁石を内蔵し、所望によつては該永久
磁石にフオーカス調整用電圧を加えることによつ
て、電界レンズおよび磁界レンズよりなる複合電
子レンズを構成し、球面収差などを補正すること
ができるので、容易にけい光面上に収差の少ない
焦点を正しく結ばせ、高解像度の映像を形成させ
る事が可能となる。従つて従来の真空外囲器外に
電磁集束コイルを用いていたものに比べ重量、体
積およびコストが大幅に改善出き、しかも従来あ
つた集束コイル用回路も省略出来る。また本明細
書でいう導電性永久磁石は、前述のように材質そ
のものが導電性であるものに限定されるものでは
なく、その表面を導電性化されたものをも含むこ
とは明らかである。
As described above, in the present invention, a conductive permanent magnet is built in the vacuum envelope, and if desired, by applying a focus adjustment voltage to the permanent magnet, an electric field lens and a magnetic field lens can be formed. Since a composite electron lens can be configured and spherical aberration can be corrected, it is possible to easily focus correctly on a phosphorescent surface with little aberration and form a high-resolution image. Therefore, the weight, volume and cost can be significantly improved compared to the conventional vacuum envelope which uses an electromagnetic focusing coil outside the vacuum envelope, and furthermore, the conventional focusing coil circuit can be omitted. Furthermore, it is clear that the conductive permanent magnet referred to in this specification is not limited to those whose material itself is conductive as described above, but also includes those whose surfaces are made conductive.

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

第1図は従来の磁界集束方式の陰極線管電子銃
の概略図、第2図および第3図はそれぞれ本発明
の概略図である。 1……真空外囲器、3……カソード電極、4…
…第1グリツド電極、5……第2グリツド電極、
6……第3グリツド電極、7b,7c……永久磁
石、8……第4グリツド電極。
FIG. 1 is a schematic diagram of a conventional magnetic field focusing type cathode ray tube electron gun, and FIGS. 2 and 3 are schematic diagrams of the present invention. 1... Vacuum envelope, 3... Cathode electrode, 4...
...first grid electrode, 5...second grid electrode,
6... Third grid electrode, 7b, 7c... Permanent magnet, 8... Fourth grid electrode.

Claims (1)

【特許請求の範囲】 1 真空外囲器内に配置されたカソード電極と、
カソード電極から放出された電子ビームを集束す
るための複数のグリツド電極とを有する陰極線管
電子銃において、少なくとも1つのグリツド電極
の少なくとも一部を、導電性の円筒型永久磁石で
構成し、その内部に磁界レンズを形成すると共
に、これに所定の電圧を印加して、隣接するグリ
ツド電極との間の間隙部に電界レンズを形成する
ことを特徴とする陰極線管電子銃。 2 導電性永久磁石にフオーカス調整用電圧を印
加することを特徴とする前記特許請求の範囲第1
項記載の陰極線管電子銃。
[Claims] 1. A cathode electrode disposed within a vacuum envelope;
In a cathode ray tube electron gun having a plurality of grid electrodes for focusing an electron beam emitted from a cathode electrode, at least a part of at least one grid electrode is composed of a conductive cylindrical permanent magnet, and the inside thereof is 1. A cathode ray tube electron gun characterized in that a magnetic field lens is formed in the gap between adjacent grid electrodes, and an electric field lens is formed in the gap between adjacent grid electrodes by applying a predetermined voltage to the magnetic field lens. 2. Claim 1, characterized in that a focus adjustment voltage is applied to the conductive permanent magnet.
The cathode ray tube electron gun described in Section 1.
JP15242277A 1977-12-20 1977-12-20 Cathode-ray tube electron gun Granted JPS5484966A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15242277A JPS5484966A (en) 1977-12-20 1977-12-20 Cathode-ray tube electron gun

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15242277A JPS5484966A (en) 1977-12-20 1977-12-20 Cathode-ray tube electron gun

Publications (2)

Publication Number Publication Date
JPS5484966A JPS5484966A (en) 1979-07-06
JPS6138574B2 true JPS6138574B2 (en) 1986-08-29

Family

ID=15540159

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15242277A Granted JPS5484966A (en) 1977-12-20 1977-12-20 Cathode-ray tube electron gun

Country Status (1)

Country Link
JP (1) JPS5484966A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60180045A (en) * 1984-02-24 1985-09-13 Matsushita Electronics Corp Method of manufacturing cathode ray tube

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5026274U (en) * 1973-07-03 1975-03-26

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5026274U (en) * 1973-07-03 1975-03-26

Also Published As

Publication number Publication date
JPS5484966A (en) 1979-07-06

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