JPH0524607B2 - - Google Patents
Info
- Publication number
- JPH0524607B2 JPH0524607B2 JP58164636A JP16463683A JPH0524607B2 JP H0524607 B2 JPH0524607 B2 JP H0524607B2 JP 58164636 A JP58164636 A JP 58164636A JP 16463683 A JP16463683 A JP 16463683A JP H0524607 B2 JPH0524607 B2 JP H0524607B2
- Authority
- JP
- Japan
- Prior art keywords
- focusing
- tube
- magnetic field
- cathode ray
- phosphor screen
- 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 - Lifetime
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J29/00—Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
- H01J29/46—Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
- H01J29/58—Arrangements for focusing or reflecting ray or beam
- H01J29/64—Magnetic lenses
- H01J29/68—Magnetic lenses using permanent magnets only
Landscapes
- Manufacture Of Electron Tubes, Discharge Lamp Vessels, Lead-In Wires, And The Like (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、小型陰極線管とくに電子ビームを静
電的かつ磁気的に集束する機能を備えた超小型陰
極線管の製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a method for manufacturing a miniature cathode ray tube, particularly a microcathode ray tube having a function of electrostatically and magnetically focusing an electron beam.
従来例の構成とその問題点
ビデオカメラのビユーフアインダとして、スク
リーン面対角線長が1.5インチ、1インチまたは
0.5インチ程度の超小型陰極線管が用いられてい
る。かかる陰極線管は多くの場合、電池により駆
動されるので、とくに小消費電力で高能率動作を
することが望まれる。Conventional configuration and its problems As a video camera viewfinder, the diagonal length of the screen surface is 1.5 inches, 1 inch or 1 inch.
Ultra-compact cathode ray tubes of about 0.5 inches are used. Since such cathode ray tubes are often powered by batteries, it is especially desirable that they operate with low power consumption and high efficiency.
前述のような超小型陰極線管における偏向電力
は、全消費電力に対してかなりの割合を占めるの
で、偏向電力の軽減が省電力化に大きく寄与す
る。偏向電力は陽極電圧に比例するので、陽極電
圧を下げると偏向電力を軽減させ得るが、単に陽
極電圧を下げると螢光体スクリーン面に必要な輝
度を得ることが困難になる。螢光体スクリーン面
にメタルバツクを有しない陰極線管では、比較的
低い陽極電圧で必要なスクリーン面輝度を得るこ
とができるが、螢光体スクリーン面にいわゆるイ
オン焼けを生じる。また、メタルバツクを構成す
るアルミニウム蒸着膜の膜厚を小さくしても陽極
電圧を下げ得るが、この膜厚をたとえば半減させ
て0.03μmに設定したものにおけるスクリーン面
輝度(陽極電圧2KV)は、メタルバクを有しな
い場合のスクリーン面輝度(陽極電圧2KV)に
比べて概ね半分となり、十分とは云えない。 Since the deflection power in the above-mentioned ultra-small cathode ray tube occupies a considerable proportion of the total power consumption, reducing the deflection power greatly contributes to power saving. Since the deflection power is proportional to the anode voltage, lowering the anode voltage can reduce the deflection power, but simply lowering the anode voltage makes it difficult to obtain the necessary brightness on the phosphor screen surface. In cathode ray tubes that do not have a metal back on the phosphor screen surface, the required screen surface brightness can be obtained with a relatively low anode voltage, but so-called ion burn occurs on the phosphor screen surface. Also, the anode voltage can be lowered by reducing the thickness of the aluminum vapor-deposited film constituting the metal back; The screen surface brightness is approximately half that of the case without the screen (anode voltage 2KV), which cannot be said to be sufficient.
さらに、前記膜厚を小さくすると、膜面にしわ
が模様状に生じる。そしてビユーフアインダのよ
うに光学レンズを通して螢光体スクリーン面を眺
める場合、前記しわが非常に見苦しいものとな
る。 Furthermore, when the film thickness is reduced, wrinkles are formed on the film surface in a pattern. When viewing the phosphor screen surface through an optical lens as in a viewfinder, the wrinkles become very unsightly.
発明の目的
本発明の目的は、メタルバツクを具備しないで
イオン焼けをほとんど生じない高能率・高品位小
型陰極線管を得るのに適した製造方法を提供する
ことにある。OBJECTS OF THE INVENTION An object of the present invention is to provide a manufacturing method suitable for obtaining a high-efficiency, high-quality compact cathode ray tube that does not include a metal bag and hardly causes ion burnout.
発明の構成
本発明の製造方法によると、静電集束型電子銃
の陰極と偏向ヨークとの間に配設されて電子ビー
ム集束磁界を発生する磁性体リングを、管内排気
後に着磁処理するのであり、これを以下図面に示
した実施例とともに詳しく説明する。Structure of the Invention According to the manufacturing method of the present invention, the magnetic ring that is disposed between the cathode and the deflection yoke of an electrostatic focusing electron gun and generates an electron beam focusing magnetic field is magnetized after the tube is evacuated. This will be explained in detail below along with the embodiments shown in the drawings.
第1図においてガラスバルブ1のネツク部2に
封入されている静電集束型電子銃3は、陰極4、
制御電極5、加速電極6、集束電極7および陽極
8を備えてなるとともに、集束電極7の内周面に
強磁性体リング9を付設している。強磁性体リン
グ9は銃軸と同軸になるように配置されており、
銃軸方向にS、N極が生じるように着磁されるこ
とにより、銃軸と同軸の電子ビーム集束用磁界を
生成する。 In FIG. 1, an electrostatic focusing electron gun 3 enclosed in a neck portion 2 of a glass bulb 1 has a cathode 4,
It comprises a control electrode 5, an acceleration electrode 6, a focusing electrode 7, and an anode 8, and a ferromagnetic ring 9 is attached to the inner peripheral surface of the focusing electrode 7. The ferromagnetic ring 9 is arranged coaxially with the gun axis,
By being magnetized so that S and N poles are generated in the direction of the gun axis, a magnetic field for electron beam focusing coaxial with the gun axis is generated.
一方、ガラスバルブ1のフエースパネル部10
の内面に付設されている螢光体スクリーン11は
メタルバツクを具備しておらず、電子銃3とはメ
タルバツクを介することなく向き合つている。1
2は陽極8と同電位に保持される内部導電膜、1
3は偏向ヨークを示す。 On the other hand, the face panel portion 10 of the glass bulb 1
The phosphor screen 11 attached to the inner surface of the phosphor screen 11 does not have a metal back and faces the electron gun 3 without a metal back. 1
2 is an internal conductive film held at the same potential as the anode 8;
3 indicates a deflection yoke.
電子銃3から放射された変調電子ビームは、偏
向ヨーク13による水平および垂直偏向磁界によ
つて偏向作用を受け、螢光体スクリーン11の面
上にモノクローム画像を映出するのであるが、集
束電極7に射入した変調電子ビームは、着磁され
た強磁性体リング9による集束用磁界で予備集束
されたのち、集束電極7と陽極8との間に生成さ
れる主電子レンズにより最終的な集束作用を受け
る。すなわち、集束電極7に射入した変調電子ビ
ームは、前記集束用磁界と前記主電子レンズとに
より2段集束されることになる。 The modulated electron beam emitted from the electron gun 3 is deflected by the horizontal and vertical deflection magnetic fields produced by the deflection yoke 13, and a monochrome image is projected on the surface of the phosphor screen 11. The modulated electron beam incident on 7 is prefocused by a focusing magnetic field produced by a magnetized ferromagnetic ring 9, and then finally focused by a main electron lens generated between the focusing electrode 7 and anode 8. Receives a focusing effect. That is, the modulated electron beam incident on the focusing electrode 7 is focused in two stages by the focusing magnetic field and the main electron lens.
一方、制御電極5と加速電極6との間のクロス
オーバ付近で生じた陰イオンは、電子ビームと同
様に前記主レンズにより集束されるが、電子に比
して質量が大きいため、強磁性体リング9による
集束磁界および偏向ヨーク13による偏向磁界の
影響はほとんど受けない。したがつて前記主レン
ズにより不完全に集束された陰イオンは螢光体ス
クリーン11の中心部を中心とする比較的広い領
域に射突し、螢光体スクリーンの中心部にのみイ
オン焼けを生じることがない。 On the other hand, negative ions generated near the crossover between the control electrode 5 and the accelerating electrode 6 are focused by the main lens in the same way as the electron beam, but since they have a large mass compared to the electrons, they are made of ferromagnetic material. It is hardly affected by the focusing magnetic field by the ring 9 and the deflection magnetic field by the deflection yoke 13. Therefore, the anions incompletely focused by the main lens impinge on a relatively wide area centered on the center of the phosphor screen 11, causing ion burn only in the center of the phosphor screen. Never.
これを第2図によりさらに詳しく説明すると、
同図に実線で示す電子ビーム14は、強磁性体リ
ング9による磁界レンズ15および主電子レンズ
16により集束されて螢光体スクリーン11の面
上の一点に収斂するのに対し、破線で示す陰イオ
ンビーム17は主として主電子レンズ16のみで
集束されるため、螢光体スクリーン11の面上の
一点に収斂せず、比較的広い領域に分散する。こ
のため、メタルバツクを有していないにもかかわ
らずイオン焼けを生じることがかなり緩和され
る。 To explain this in more detail using Figure 2,
The electron beam 14 shown by the solid line in the same figure is focused by the magnetic field lens 15 formed by the ferromagnetic ring 9 and the main electron lens 16 and converges to a point on the surface of the phosphor screen 11, whereas the electron beam 14 is shown by the shadow shown by the broken line. Since the ion beam 17 is mainly focused only by the main electron lens 16, it does not converge to a single point on the surface of the phosphor screen 11, but is dispersed over a relatively wide area. For this reason, the occurrence of ion burn is considerably reduced even though it does not have a metal back.
なお、前記実施例では強磁性体リング9を集束
電極7の内周面に付設したが、同電極7の外周面
上に同軸的に設けてもよい。また、強磁性体リン
グ9は必ずしも集束電極7に付設する必要はな
く、要するに、陰極4と偏向ヨーク13との中間
点付近における管内に同軸的に設置されておれば
よい。 Although the ferromagnetic ring 9 is attached to the inner circumferential surface of the focusing electrode 7 in the embodiment described above, it may be coaxially provided on the outer circumferential surface of the focusing electrode 7. Further, the ferromagnetic ring 9 does not necessarily need to be attached to the focusing electrode 7, and in short, it is sufficient if it is coaxially installed in the tube near the midpoint between the cathode 4 and the deflection yoke 13.
ところで、強磁性体リング9を含む電子銃構成
部材は、管内排気工程中にガス抜きのために約
400℃の温度に加熱される。その上、この加熱の
温度分布は必ずしも一様でないので、予め着磁さ
れている強磁性体リング9の保磁力が、管内排気
工程の前後で不規則的に変化することがある。そ
してこのようなことがあると、予定のイオン分散
効果および電子ビーム集束効果を満足に得ること
が困難になる。 By the way, the electron gun components including the ferromagnetic ring 9 are used for gas removal during the tube exhaust process.
Heated to a temperature of 400℃. Furthermore, since the temperature distribution of this heating is not necessarily uniform, the coercive force of the ferromagnetic ring 9, which has been magnetized in advance, may change irregularly before and after the pipe evacuation process. If this happens, it becomes difficult to obtain the intended ion dispersion effect and electron beam focusing effect satisfactorily.
そこで本発明では、強磁性体リング9に対する
着磁処理を管内排気後に行なう。第3図に示す着
磁処理装置18は、コ字状鉄片19とこれに巻装
されたコイル20とからなり、コイル20に直流
電流を通じることによつて1対の磁極部21,2
2間に着磁用磁界23が発生する。そして、磁界
23に管軸が平行となるように配置された排気後
の被処理陰極線管24の強磁性体リングが磁界2
3により所定の保磁力に着磁される。 Therefore, in the present invention, the magnetization process for the ferromagnetic ring 9 is performed after the tube is evacuated. The magnetization processing device 18 shown in FIG. 3 consists of a U-shaped iron piece 19 and a coil 20 wound around it.
A magnetizing magnetic field 23 is generated between the two. Then, the ferromagnetic ring of the cathode ray tube 24 to be processed after exhaust, which is arranged so that the tube axis is parallel to the magnetic field 23, is exposed to the magnetic field 23.
3, it is magnetized to a predetermined coercive force.
完成した陰極線管を作動させてみて電子ビーム
の集束状態が最適でない場合は、装置18で再着
磁または減磁をすればよい。 When operating the completed cathode ray tube, if the focused state of the electron beam is not optimal, the device 18 may be used to re-magnetize or demagnetize it.
発明の効果
本発明の小型陰極線管製造方法は前述のように
構成されるので、比較的低い陽極電圧で十分な輝
度が得られ、しかもイオン焼けの心配がほとんど
ない高能率小型陰極線管を得ることができるのみ
ならず、強磁性体リングの着磁および保磁力の一
様性が得られ、電子ビーム集束磁界のばらつきや
変化による解像度の低下が防止される。Effects of the Invention Since the method for manufacturing a small cathode ray tube of the present invention is configured as described above, it is possible to obtain a high efficiency small cathode ray tube that can obtain sufficient brightness with a relatively low anode voltage and has almost no fear of ion burnout. Not only this, but also the uniformity of the magnetization and coercive force of the ferromagnetic ring can be obtained, and a decrease in resolution due to variations and changes in the electron beam focusing magnetic field can be prevented.
第1図は本発明の対象となる小型陰極線管の側
断面図、第2図は同陰極線管の強磁性体リングに
よる磁界レンズと主電子レンズとの動作説明図、
第3図は本発明の製造方法において適用される着
磁処理装置の1例を示す斜視図である。
3……電子銃、4……陰極、7……集束電極、
9……強磁性体リング、11……螢光体スクリー
ン、13……偏向ヨーク。
FIG. 1 is a side cross-sectional view of a small cathode ray tube to which the present invention is applied, and FIG. 2 is an explanatory diagram of the operation of a magnetic field lens and a main electron lens formed by a ferromagnetic ring of the same cathode ray tube.
FIG. 3 is a perspective view showing an example of a magnetization processing apparatus applied in the manufacturing method of the present invention. 3... Electron gun, 4... Cathode, 7... Focusing electrode,
9... Ferromagnetic ring, 11... Fluorescent screen, 13... Deflection yoke.
Claims (1)
ツクを介することなく向き合う蛍光体スクリーン
と、前記電子銃の陰極と偏向ヨークとの間におけ
る管内部分に配設されて管軸に略平行な電子ビー
ム集束用磁界を発生する磁性体リングとを備えて
なる小型陰極線管の製造において、前記磁性体リ
ングを管内排気後に着磁処理することを特徴とす
る小型陰極線管の製造方法。1 An electrostatic focusing electron gun, a phosphor screen that faces the electron gun without intervening a metal bag, and an electron beam disposed in the tube between the cathode and the deflection yoke of the electron gun and arranged approximately parallel to the tube axis. 1. A method of manufacturing a small cathode ray tube comprising a magnetic ring that generates a beam focusing magnetic field, the method comprising magnetizing the magnetic ring after the tube is evacuated.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58164636A JPS6056338A (en) | 1983-09-07 | 1983-09-07 | Manufacture of small size cathode ray tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58164636A JPS6056338A (en) | 1983-09-07 | 1983-09-07 | Manufacture of small size cathode ray tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6056338A JPS6056338A (en) | 1985-04-01 |
| JPH0524607B2 true JPH0524607B2 (en) | 1993-04-08 |
Family
ID=15796957
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58164636A Granted JPS6056338A (en) | 1983-09-07 | 1983-09-07 | Manufacture of small size cathode ray tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6056338A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5632640A (en) * | 1979-08-27 | 1981-04-02 | Nec Corp | Manufacture of cathode-ray tube |
| JPS57167558U (en) * | 1981-04-15 | 1982-10-22 |
-
1983
- 1983-09-07 JP JP58164636A patent/JPS6056338A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6056338A (en) | 1985-04-01 |
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