JPH039241Y2 - - Google Patents

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Publication number
JPH039241Y2
JPH039241Y2 JP1983131017U JP13101783U JPH039241Y2 JP H039241 Y2 JPH039241 Y2 JP H039241Y2 JP 1983131017 U JP1983131017 U JP 1983131017U JP 13101783 U JP13101783 U JP 13101783U JP H039241 Y2 JPH039241 Y2 JP H039241Y2
Authority
JP
Japan
Prior art keywords
electrode
tube
electron
heating
slit
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
JP1983131017U
Other languages
Japanese (ja)
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JPS6039551U (en
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
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Priority to JP13101783U priority Critical patent/JPS6039551U/en
Publication of JPS6039551U publication Critical patent/JPS6039551U/en
Application granted granted Critical
Publication of JPH039241Y2 publication Critical patent/JPH039241Y2/ja
Granted legal-status Critical Current

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  • Image-Pickup Tubes, Image-Amplification Tubes, And Storage Tubes (AREA)

Description

【考案の詳細な説明】 本考案は、熱陰極を備えた電子管に関する。更
に詳述すれば、本考案は受像管などの陰極線管、
撮像管およびその他の電子管を製作する工程にお
いて不可欠な高周波加熱による電極類のガス出し
を、所要の高温にて可能ならしめ、もつて安定な
カソードエミツシヨンが得られるようにした電極
構造を提供するものである。
[Detailed Description of the Invention] The present invention relates to an electron tube equipped with a hot cathode. More specifically, the present invention applies to cathode ray tubes such as picture tubes,
Provides an electrode structure that enables degassing of electrodes at the required high temperature through high-frequency heating, which is essential in the process of manufacturing image pickup tubes and other electron tubes, and that also provides stable cathode emission. It is something to do.

第1図は、従来から知られている小型のMS型
撮像管の一例を示す。電子管のひとつである撮像
管を製作するに際して必要な排気を行うために、
チツプ管1を真空ポンプ(図示せず)に取り付け
る。そして、管内を10-7Torr前後の高真空に引
きながら、G1電極5あるいはG2電極6などの電
極を加熱する高周波加熱用コイル2により管内の
電極を順次数100℃に加熱し、それにより電極の
吸蔵ガスを十分排出せしめ、しかる後に、カソー
ド(図示せず)に組み込まれたヒータにより加熱
して熱電子放出面を活性化していく方法がとられ
ている。
FIG. 1 shows an example of a conventionally known small MS type image pickup tube. In order to perform the exhaust necessary when manufacturing an image pickup tube, which is one of the electron tubes,
Attach the tip tube 1 to a vacuum pump (not shown). Then, while drawing a high vacuum around 10 -7 Torr inside the tube, the high-frequency heating coil 2 that heats the electrodes such as the G1 electrode 5 or the G2 electrode 6 sequentially heats the electrodes in the tube to several 100 degrees Celsius. A method is used in which the absorbed gas is sufficiently discharged, and then the cathode (not shown) is heated by a heater incorporated in the cathode to activate the thermionic emission surface.

かかる排気プロセスが完了したあとは、チツプ
管1は溶融・切断され、高周波加熱によりゲツタ
3がガラス外管4の内面に蒸着せしめられる。こ
こで、電極を加熱するための高周波加熱用コイル
2から発生する高周波磁束10はコイルの両端に
おいて広がつていくので、加熱範囲は高周波コイ
ル2の長さlの範囲にとどまらず、高周波加熱用
コイル2の上下にわたる広範囲(数mm〜数10mm)
に及ぶ。
After the evacuation process is completed, the chip tube 1 is melted and cut, and the getter 3 is deposited on the inner surface of the glass outer tube 4 by high frequency heating. Here, the high-frequency magnetic flux 10 generated from the high-frequency heating coil 2 for heating the electrode spreads at both ends of the coil, so the heating range is not limited to the length l of the high-frequency coil 2; Wide range above and below coil 2 (several mm to several tens of mm)
It extends to.

したがつて、不要の個所を加熱しないようにす
るために、加熱防止板16を高周波加熱用コイル
2の上に密着して配置し、加熱範囲の制御が行わ
れている。
Therefore, in order to avoid heating unnecessary areas, a heating prevention plate 16 is disposed in close contact with the high-frequency heating coil 2 to control the heating range.

ところが実際には、電子光学的な必要から種々
の形状を有する電極をそれぞれ別個の位置に配置
しなければならないので、場合によつては各々の
電極における加熱温度に極端な差が生じてしまう
という不都合がみられる。殊に、高品位テレビジ
ヨン用の撮像管などは外管4の直径が従来のもの
に比べて大であるので、かかる加熱度の差異は顕
著なものとなる。このように、従来から行われて
いる加熱・排気処理では、電極の最高加熱温度が
最も加熱されやすい電極によつて制限されてしま
うので、他の電極のベーキング温度を上げること
ができなくなる。その結果、十分な電極のガス出
しが不能になり、あるいは長時間を要することに
なつて、長期安定なエミツシヨンを確保するため
のカソード活性化が不可能もしくは不十分となつ
てしまうという欠点がある。
However, in reality, electrodes with various shapes must be placed in separate positions due to electro-optical requirements, which can lead to extreme differences in the heating temperature of each electrode. There are some inconveniences. In particular, since the diameter of the outer tube 4 of an image pickup tube for high-definition television is larger than that of a conventional tube, the difference in the degree of heating becomes significant. In this manner, in the conventional heating and exhaust treatment, the maximum heating temperature of the electrode is limited by the electrode that is most easily heated, making it impossible to increase the baking temperature of other electrodes. As a result, sufficient gas release from the electrode becomes impossible or takes a long time, making it impossible or insufficient to activate the cathode to ensure long-term stable emission. .

本考案の目的は、かかる電極配置もしくは電極
構造をもつ電子管に対し、各電極の均一加熱を可
能ならしめ、安定かつ高効率なカソードエミツシ
ヨンを確保するようにした電極構造を有する電子
管を提供することにある。
The purpose of the present invention is to provide an electron tube having such an electrode arrangement or structure that enables uniform heating of each electrode and ensures stable and highly efficient cathode emission. It's about doing.

かかる目的を達成するために、本考案では電子
ビームを通過させるための中央開口部を設けた複
数個の電極を有する電子管において、少くとも1
個の電極にスリツトを設けるよう構成する。
In order to achieve this purpose, the present invention provides an electron tube having a plurality of electrodes each having a central opening through which an electron beam passes.
The structure is such that a slit is provided in each electrode.

以下に、図面を参照して本考案を詳細に説明す
る。
Hereinafter, the present invention will be described in detail with reference to the drawings.

ここでは、第1図示のMS型撮像管に本考案を
適用した一実施例について説明する。
Here, an embodiment will be described in which the present invention is applied to the MS type image pickup tube shown in the first figure.

第1図において、5はG1電極、6はG2電極、
12は外管4の内面に蒸着された金属薄膜を加工
したデフレクトロン電極、13はターゲツトから
の戻り電子ビームを吸収することを主目的とした
中央開口部付き反射板電極、14は電子銃ブロツ
ク(G1電極5およびG2電極6を含む)と外管4
とを軸合せして取付けるための絶縁物よりなる保
持体である。
In Figure 1, 5 is the G1 electrode, 6 is the G2 electrode,
12 is a deflectron electrode made of a metal thin film deposited on the inner surface of the outer tube 4; 13 is a reflector electrode with a central opening whose main purpose is to absorb the electron beam returning from the target; 14 is an electron gun block. (including G1 electrode 5 and G2 electrode 6) and outer tube 4
This is a holder made of insulating material for aligning and installing.

反射板電極13としては電子光学的な必要か
ら、外管4の内径d4にほぼ等しい直径をもつ円板
状電極を用いるが、他の電極は直径がd4/2程度
の円筒状電極もしくは片方にふたを設けた円筒状
電極を用いる。
As the reflector electrode 13, a disk-shaped electrode with a diameter approximately equal to the inner diameter d 4 of the outer tube 4 is used due to electro-optical requirements, but the other electrodes are cylindrical electrodes with a diameter of about d 4 /2 or A cylindrical electrode with a lid on one end is used.

これら電極の板厚は、均一加熱への配慮から全
電極ともほぼ等しく、例えば0.2mm前後のものを
用いる。
The plate thickness of these electrodes is approximately equal for all electrodes, for example, approximately 0.2 mm in consideration of uniform heating.

一般に、加熱範囲および加熱温度の制御は、高
周波加熱用コイル2の長さl、巻数、直径d1、巻
線の直径d5、並びに加熱防止板16の厚さl1、内
径d6、材質などを適切に選択することにより行
う。しかし、本出願人による実験によれば、撮像
管電極の直径に2倍以上の差が存在する場合に
は、直径の大きい電極と小さい電極との間におい
て加熱バランスをとることは不可能であることが
確認された。
Generally, the heating range and heating temperature are controlled by the length l, number of turns, diameter d 1 , diameter d 5 of the winding of the high-frequency heating coil 2, and the thickness l 1 , inner diameter d 6 , and material of the heating prevention plate 16. This is done by appropriately selecting the following. However, according to experiments conducted by the applicant, if there is a difference of two or more times in the diameter of the image pickup tube electrodes, it is impossible to maintain a heating balance between the larger diameter electrode and the smaller diameter electrode. This was confirmed.

例えば、高品位テレビジヨン用の高解像度1イ
ンチMS型撮像管では、反射板電極13の直径は
23mm、他の電極群の直径は8mmであるが、この場
合、反射板電極と他の電極群との間には約200℃
の温度差が生じた。
For example, in a high-resolution 1-inch MS type image pickup tube for high-definition television, the diameter of the reflector electrode 13 is
The diameter of the other electrode group is 8 mm, but in this case, there is a temperature of about 200°C between the reflector electrode and the other electrode group.
A temperature difference of .

かかる欠点を排除するために本考案の一実施例
では、第2図AおよびBに示すように、直径が大
である方の電極(例えば、円板状の反射板電極1
3)の中央に電子ビームを通過させるための中央
開口部を設けるほか、スリツト25を新たに設け
る。すなわち、第2図Aは反射板電極13に中央
開口部のほか、これと連結した1個のスリツトを
設けた実施例を示す。また、第2図Bは同電極に
中央開口部のほか独立に複数個のスリツトを設
け、該スリツトを電極13の縁まで切欠いてオー
プン構造とした別実施例を示す。
In order to eliminate such drawbacks, in one embodiment of the present invention, as shown in FIGS.
3) In addition to providing a central opening for the electron beam to pass through, a slit 25 is newly provided. That is, FIG. 2A shows an embodiment in which the reflecting plate electrode 13 is provided with a central opening and one slit connected to the central opening. Further, FIG. 2B shows another embodiment in which the same electrode is provided with a plurality of independent slits in addition to the central opening, and the slits are cut out to the edge of the electrode 13 to form an open structure.

ここで、スリツトの形状、大きさ、本数などは
所望のベーキング温度が得られるよう必要に応じ
て最適な形状を選択する。
Here, the optimum shape, size, number, etc. of the slits are selected as necessary so as to obtain the desired baking temperature.

このように反射板電極13に中央開口部以外に
スリツトを設けると、高周波磁界に起因して生じ
る渦電流が妨げられるので、ジユール熱の発生に
よる電極の焼けすぎを防止することができる。そ
の結果、電子光学的な必要から加熱・排気中に異
常加熱を受けざるを得ない電極構造をもつ小型撮
像管あるいはその他の電子管に対しても、その加
熱・排気処理中、高周波による加熱条件を揃えて
電極のガス出しを行うことが可能となる。従つ
て、カソードの活性化を理想的な条件で行うこと
ができ、もつてカソードの長期安定なエミツシヨ
ンを容易に確保することができる。
When the reflector electrode 13 is provided with a slit other than the central opening in this manner, eddy currents generated due to the high frequency magnetic field are prevented, so that over-burning of the electrode due to generation of Joule heat can be prevented. As a result, even for small image pickup tubes or other electron tubes with electrode structures that are forced to undergo abnormal heating during heating and exhaust due to electro-optical requirements, high-frequency heating conditions are required during heating and exhausting. It becomes possible to vent gas from the electrodes in alignment. Therefore, activation of the cathode can be performed under ideal conditions, and long-term stable emission of the cathode can be easily ensured.

例えば、上述した高品位テレビジヨン用MS型
撮像管に超高解像度のBI(Barium
Impregnated)カソードを用いた電子銃を組み込
むと共に、反射板電極13の直径を23mm、電子銃
部(G1電極5およびG2電極6)の直径を8mm前
後とした場合には、本考案に係るスリツト25を
反射板電極13に付加しないと、反射板電極を
700℃前後に加熱しても、この電子銃部は500℃以
下にしか加熱し得なかつた。その結果、所望のカ
ソードエミツシヨンは設計値の数分の1以下しか
確保することができなかつた。
For example, the ultra-high resolution BI (Barium
When an electron gun using a cathode (Impregnated) is incorporated, and the diameter of the reflector electrode 13 is 23 mm and the diameter of the electron gun part (G1 electrode 5 and G2 electrode 6) is about 8 mm, the slit 25 according to the present invention If not added to the reflector electrode 13, the reflector electrode
Even when heated to around 700°C, this electron gun could only be heated to below 500°C. As a result, the desired cathode emission could only be secured to a fraction of the design value.

しかし、第2図Aに示したスリツトを反射板電
極13に設けることによつて、全電極をほぼ所望
の700℃前後に加熱することができ、エミツシヨ
ンの設計値(すなわち、数A/cm2以上)を安定し
て確保することができた。
However, by providing the slits shown in FIG. 2A in the reflector electrode 13, the entire electrode can be heated to approximately the desired temperature of 700°C, and the design value of the emission (i.e., several A/cm 2 above) were able to be stably secured.

なお、以上述べた説明から明らかなように、本
考案はMS型もしくはMM型撮像管のみならず、
異なつた大きさの電極を有するその他の電子管全
てに、広く適用できることは勿論である。
As is clear from the above explanation, the present invention is applicable not only to MS type or MM type image pickup tubes.
Of course, it is widely applicable to all other electron tubes having electrodes of different sizes.

以上説明したとおり、本考案によれば、中央開
口部を有する電極にスリツトを設けて渦電流によ
る発熱を防止することができるので、種々の形状
ないし配置を有する電極を均一の温度にて加熱す
ることが可能となり、もつてカソードの良好なエ
ミツシヨン特性を得ることができる。
As explained above, according to the present invention, it is possible to prevent heat generation due to eddy current by providing a slit in an electrode having a central opening, so that electrodes having various shapes or arrangements can be heated at a uniform temperature. This makes it possible to obtain good emission characteristics of the cathode.

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

第1図は従来から知られている小型のMS型撮
像管を示す断面構成図、第2図A,Bはそれぞれ
本考案の一実施例によるスリツト付き円板状電極
を示す平面図である。 1……チツプ管、2……高周波加熱用コイル、
3……ゲツタ、4……外管、5……G1電極、6
……G2電極、9……インジウムリング、10…
…磁力線、12……デフレクトロン、13……反
射板電極、14…保持体、15……ステム、16
……加熱防止板、17……ステムと電子銃との間
の空間、18……ステムピン、25……スリツ
ト。
FIG. 1 is a cross-sectional configuration diagram showing a conventionally known small MS type image pickup tube, and FIGS. 2A and 2B are plan views each showing a disc-shaped electrode with a slit according to an embodiment of the present invention. 1...Chip tube, 2...High frequency heating coil,
3...Getter, 4...Outer tube, 5...G1 electrode, 6
...G2 electrode, 9...Indium ring, 10...
... Lines of magnetic force, 12 ... Deflectron, 13 ... Reflection plate electrode, 14 ... Holder, 15 ... Stem, 16
... Heating prevention plate, 17 ... Space between stem and electron gun, 18 ... Stem pin, 25 ... Slit.

Claims (1)

【実用新案登録請求の範囲】 1 真空外囲管の所定部位に向けて電子ビームを
発射させる電子銃ブロツクと、 前記外囲管の所定部位に設けられたターゲツ
トと、 前記電子銃ブロツクから前記ターゲツトに至
る電子ビームを通過させるための中央開口部を
有すると共に、管軸に対して放射状のスリツト
を有する円板状もしくは円筒状の電極と、 を備え、前記外囲管の外側から前記電極を加熱
するための高周波加熱用コイルに通電した時生
じる渦電流を、前記スリツトによつて低減させ
ることを特徴とする電子管。 2 前記電極に設けられている前記中央開口部と
前記スリツトとを連結させた構造としたことを
特徴とする実用新案登録請求の範囲第1項に記
載の電子管。 3 前記電極に設けられている前記スリツトを、
該電極の外周部に至るまで延長させたオープン
構造としたことを特徴とする実用新案登録請求
の範囲第1項に記載の電子管。
[Claims for Utility Model Registration] 1. An electron gun block that emits an electron beam toward a predetermined portion of a vacuum envelope tube, a target provided at a predetermined portion of the envelope tube, and a target from the electron gun block. a disk-shaped or cylindrical electrode having a central opening for passing an electron beam reaching the tube axis and having slits radial to the tube axis; An electron tube characterized in that the slit reduces eddy currents that occur when electricity is applied to a high-frequency heating coil for heating. 2. The electron tube according to claim 1, which is a registered utility model, characterized in that the central opening provided in the electrode is connected to the slit. 3. The slit provided in the electrode,
The electron tube according to claim 1, which has been registered as a utility model, is characterized in that it has an open structure extending to the outer periphery of the electrode.
JP13101783U 1983-08-26 1983-08-26 electron tube Granted JPS6039551U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13101783U JPS6039551U (en) 1983-08-26 1983-08-26 electron tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13101783U JPS6039551U (en) 1983-08-26 1983-08-26 electron tube

Publications (2)

Publication Number Publication Date
JPS6039551U JPS6039551U (en) 1985-03-19
JPH039241Y2 true JPH039241Y2 (en) 1991-03-07

Family

ID=30296344

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13101783U Granted JPS6039551U (en) 1983-08-26 1983-08-26 electron tube

Country Status (1)

Country Link
JP (1) JPS6039551U (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5235578A (en) * 1975-09-13 1977-03-18 Toshiba Corp Manufacturing process fo hot cathode grid control discharge tube containing hydrogen

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5235578A (en) * 1975-09-13 1977-03-18 Toshiba Corp Manufacturing process fo hot cathode grid control discharge tube containing hydrogen

Also Published As

Publication number Publication date
JPS6039551U (en) 1985-03-19

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