JPH0343932A - Electron emitting apparatus - Google Patents
Electron emitting apparatusInfo
- Publication number
- JPH0343932A JPH0343932A JP1178707A JP17870789A JPH0343932A JP H0343932 A JPH0343932 A JP H0343932A JP 1178707 A JP1178707 A JP 1178707A JP 17870789 A JP17870789 A JP 17870789A JP H0343932 A JPH0343932 A JP H0343932A
- Authority
- JP
- Japan
- Prior art keywords
- film
- electron emitting
- resistor film
- reducing
- reducing member
- 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
Links
Landscapes
- Solid Thermionic Cathode (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は、ブラウン管用の電子銃等の1000 ’C
程度の高温で効率良く電子を放射する積層型の電子放射
装置の構造に関する。[Detailed Description of the Invention] [Industrial Application Field] This invention is applicable to 1000'C electron guns for cathode ray tubes, etc.
This invention relates to the structure of a stacked electron emitting device that efficiently emits electrons at moderately high temperatures.
[従来の技術]
従来、カソード材層のようム電子放射装置を平面積層型
で製造する場合、閂えば、特公昭55−24846号公
報に記載されているように、スクリーン印刷等のいわゆ
る厚膜回路形成技術を用いて製造されていた。第2図は
このようにして製造された従来の電子放射装置を示す断
面構成図である。まず、七うミソクス基板(10)を横
取する原材料を用意し、ロール間を通す押し出し法、あ
るいはキャスティング法の印刷技術によってンート上に
所望のパタノ形状の発熱体層(11)を形成し、この発
熱体層(11)を形成した基板(10)上に絶縁体〈1
2)を形成し、さらに、この絶縁体り12〉上に、同様
々印刷手法によって、 カソード材層(13〉、 カッ
−トリー1・層〈14)、ヘースメタル層(15〉を形
成し、電子放射装置を形成する。これらの発熱体層(1
1)をはじめとする各層は各材料に焼成助剤を添加した
ペースI・を、基板(10〉上に次々と重ねてスクリー
ン印刷して形成される。スクリーン印刷1麦、高温(1
000〜2000°C)で焼成され、電子放射装置が形
成される。[Prior Art] Conventionally, when manufacturing a flat layered electron emitting device with a cathode material layer, a so-called thick film method such as screen printing is used, as described in Japanese Patent Publication No. 55-24846. It was manufactured using circuit formation technology. FIG. 2 is a cross-sectional configuration diagram showing a conventional electron emitting device manufactured in this manner. First, raw materials are prepared to take over the Nanau Misoku substrate (10), and a heating element layer (11) in a desired pattern is formed on the belt by extrusion or casting printing technology, which is passed between rolls. An insulator <1> is placed on the substrate (10) on which this heating element layer (11) is formed.
2) is formed, and furthermore, a cathode material layer (13), a cutter 1 layer (14), and a heat metal layer (15) are formed on this insulator layer (12) by the same printing method. A radiating device is formed.These heating element layers (1
Each layer including 1) is formed by screen printing Pase I, which is a mixture of materials with a baking aid added, on the substrate (10) one after another.
000-2000°C) to form an electron emitting device.
この方法では、製造時に高温処理過程が入るのでヒータ
をこの処理7m度以下で使用する場合、抵抗の経時変化
が小さい等のヒータとしての高温長期安定性か期待され
、同時にカソードも高温長期安定性が期待されていた。This method involves a high temperature treatment process during manufacturing, so if the heater is used at a temperature below 7m degrees, it is expected that the heater will have long-term stability at high temperatures, such as small changes in resistance over time, and at the same time, the cathode will also have long-term stability at high temperatures. was expected.
しかし、スクリーン印刷によって得られるパターン精度
は低く、しかも発熱体の厚さ制御(薄型化)が困難ムた
め、消費電力が大きく、しかも複数のヒータ間では抵抗
のはらつきが大きいので、カソードの電子放射も大きく
ばらつき、信頼性に欠けるものであった。そのため、精
度良くパターンの形成ができる手法としてPVDやCV
Dによる成膜法の開発が進められていた。However, the pattern accuracy obtained by screen printing is low, and it is difficult to control the thickness of the heating element (thinning it), resulting in high power consumption.Moreover, there is large variation in resistance between multiple heaters, so the cathode electron The radiation also varied widely and was unreliable. Therefore, PVD and CV are methods that can form patterns with high precision.
Development of a film forming method using D was in progress.
第3図に薄膜形成法による従来の電子放射装置を示す。FIG. 3 shows a conventional electron emitting device using a thin film formation method.
まず、平滑な七うミンクス基板上〈lO〉上にヒータ用
の抵抗体く発熱体)膜<17)を、そして反対(11]
にベースメタル用(還元部材)膜(18〉を−様に形成
し、次にエツチングにより所望のヒータパターン、カソ
ード用パターンを形成し、ベースメタル用膜の上に電子
放射部材(19)を塗布し、方これにヒータ側にはリー
ド線(20〉を接合するという手法で電子放射装置を実
現していた。First, a resistor (heating element) film <17) for a heater is placed on a smooth seven-layer substrate <lO>, and then the opposite (11)
A base metal (reducing member) film (18) is formed in a negative shape, then a desired heater pattern and cathode pattern are formed by etching, and an electron emitting member (19) is applied on the base metal film. However, an electron emitting device was realized by connecting a lead wire (20) to the heater side.
[発明か解決しようとする課題]
以上のよう/、l:成膜法による電子放射装置はIJ−
ド線に電圧を印加してヒータを加熱し、さらにセラミ・
・ノクス基板〈lO)を介してカッ−Fを加熱して電子
を放射させて使用している間に膜と基板の間で剥離か生
しる1、すムオ)ち、七うミノクス基板(10〉と抵抗
体膜<17)あるいは七うミノクス基板〈10〉とベー
スメタル用膜(18)の間で剥離が生じる。これは主と
して膜の基板への付着力が元々弱かったこと、使用時の
熱履歴により内部応力の釣CJ合いに変化が生したこと
、膜と基板との熱膨張係数が違うこと等に起因する。そ
のため剥離により熱容量に変化が生じたり、ヒータとし
ての抵抗値が変動した()、ヒータ内で断線した0、ま
た熱容量の変化に伴いカソードの電子放槍量の変動等か
起こる。さらにベースメタル(還元部材)用膜<18)
とカソード゛材とのなじみが悪く、電子放射特性が劣り
、そのためヒータ、カソードともに不安定でしかも長期
信頼性に欠け、性能も十分とは言い難いものであった。[Invention or problem to be solved] As described above, the electron emitting device using the film forming method is IJ-
A voltage is applied to the lead wire to heat the heater, and the ceramic
・During use, peeling occurs between the film and the substrate by heating Ka-F and emitting electrons through the Nox substrate (lO). Peeling occurs between the resistor film <10> and the resistor film <17) or the seven Minox substrate <10> and the base metal film (18). This is mainly due to the fact that the adhesion of the film to the substrate was originally weak, that the internal stress balance CJ changed due to the thermal history during use, and that the thermal expansion coefficients of the film and the substrate were different. . As a result, the heat capacity changes due to peeling, the resistance value as a heater fluctuates (), the wire breaks in the heater, and the amount of electrons emitted from the cathode fluctuates due to the change in heat capacity. Furthermore, base metal (reducing member) film <18)
The compatibility with the cathode material was poor, and the electron emission characteristics were poor.As a result, both the heater and the cathode were unstable, lacked long-term reliability, and their performance was far from satisfactory.
このように、電子放射装置は厚膜回路形成技術で両面に
高温で安定なポーラスな膜を設けるか、薄膜形成法によ
り付着力が小さく緻密でパターン精度の良い膜を設ける
か、の二者択一の方法で形成され、性能が十分発揮され
ていなか一つな。In this way, for electron emitting devices, there are two choices: to use thick film circuit formation technology to provide a porous film that is stable at high temperatures on both sides, or to use thin film formation technology to create a film that is dense, has low adhesion, and has good pattern accuracy. It is one of the few that has been formed using only one method, and its performance is not fully demonstrated.
この発明は、上記のような問題点を解決するためになさ
れたもので、使用時に膜と基板の剥離が生じにくく、ま
た電子放射効率の高い、信頼性の高い電子放射装置を提
供することを目的としている。This invention was made in order to solve the above-mentioned problems, and aims to provide a highly reliable electron emitting device that is less likely to cause separation between the film and the substrate during use, and has high electron emission efficiency. The purpose is
[課題を解決するための手段]
この発明に係る電子放射装置は、良熱電導性の絶縁部材
、この絶縁部材の一方の面に高融点良電気電導性材料を
用いて所定形状に形成された膜密度の高い緻密な抵抗体
膜、この抵抗体膜を覆うように形成された絶縁性保護膜
、上記絶縁部材の他方の面に良熱電導性還元材料を用い
て所定形状に形成され、上記抵抗体膜よζノ膜密度の低
い多孔質な還元部材、およびこの還元部材上で一部が還
元部材の孔に侵入して形成された電子放射部材な備えた
ものである。[Means for Solving the Problems] An electron emitting device according to the present invention includes an insulating member with good thermal conductivity, and one surface of the insulating member formed into a predetermined shape using a high melting point and good electrical conductivity material. A dense resistor film with high film density, an insulating protective film formed to cover the resistor film, and a good heat conductive reducing material formed into a predetermined shape on the other surface of the insulating member, It is equipped with a porous reducing member having a low film density than the resistor film, and an electron emitting member formed on the reducing member by partially penetrating into the pores of the reducing member.
[作用]
この発明においては、抵抗体膜を覆うように形成された
保護膜は外部雰囲気から抵抗体膜を保護するとともに使
用中に抵抗体膜が絶縁部材から剥離することを抑制する
ように作用する。また、還元部材を多孔質体で形成する
ことにより、還元部材の上に設けられた電子放射部材と
のなじみを良くし、また電子放射部材が一部還元部材へ
侵入するため、電子放射の高効率化に作用する。[Function] In the present invention, the protective film formed to cover the resistor film protects the resistor film from the external atmosphere and acts to prevent the resistor film from peeling off from the insulating member during use. do. In addition, by forming the reducing member with a porous material, it is better compatible with the electron emitting member provided on the reducing member, and since the electron emitting member partially penetrates into the reducing member, the electron emission is increased. It affects efficiency.
[実施例]
以下この発明の一実施例について図に基づいて説明する
。第1図はこの発明の一実施例による電子放射装置を示
す断面構成図である。図において、〈1)は電子放射部
材、(2〉は電子放射部材(1)を還元する膜密度の低
い多孔質体からなる還元部材(ベースメタル)であり、
電子放射部材(1)の−部が還元部材(2〉の孔に侵入
している。、(3)は電子数割部i’4’ (1)と還
元部材<2)からなるカソードを加熱するためのヒータ
用の膜密度の高い緻密ム抵抗体膜であり、高融点良電気
伝導性材料を用いて所定形状に形成されている。(4)
は還元部材(2〉とヒータ用抵抗体膜〈3〉の間に介在
し、両者を電気的に絶縁するとともにヒータ用抵抗体膜
(3)から発生された熱を還元部拐〈2〉へ効率良く伝
導−1−るための良熱伝導1生電気絶縁利料からなる絶
縁部材、〈5〉はヒータ用抵抗体膜〈3〉を葭うように
形成され抵抗体膜<3〉を外部雰囲気から保護するため
の保護膜である。[Example] An example of the present invention will be described below based on the drawings. FIG. 1 is a cross-sectional configuration diagram showing an electron emitting device according to an embodiment of the present invention. In the figure, <1) is an electron emitting member, (2> is a reducing member (base metal) made of a porous material with a low film density that reduces the electron emitting member (1),
The - part of the electron emitting member (1) has entered the hole of the reducing member (2)., (3) heats the cathode consisting of the electron fraction i'4' (1) and the reducing member <2). This is a dense resistor film with a high film density for heaters, and is formed into a predetermined shape using a high melting point and electrically conductive material. (4)
is interposed between the reducing member (2) and the heater resistor film <3>, electrically insulating the two and transferring the heat generated from the heater resistor film (3) to the reducing member (2). An insulating member <5> made of raw electrical insulation material for efficient conduction, <5>, is formed to cover the heater resistor film <3>, and the resistor film <3> is connected to the outside. It is a protective film to protect from the atmosphere.
kお、それぞれの材料に対しては、例えは、次のよう々
性質が要求される。電子放射装置の構造体である基板に
相当する絶縁部材(4)に対しては、熱伝導性か良く、
熱膨張率かヒータ用抵抗体膜〈3)および還元部材〈2
〉のそれに近いこと、長地縁体であること、高温で絶縁
破壊し々いこと、平滑なこと。そのため、入手性から考
えて八IN、 A1.203等が考えられる。ヒータ用
抵抗体膜〈3)に対しては、高温域での蒸気圧が低いこ
と、高温域での電気特性が安定なこと。そのため、Mo
、 W、 Pt、 TaTiN、 TiC,T1CN等
が考えられる。特に、再結晶温度が高く、高温で安定性
の良好に七ラミ・ノクス系のTiN、 TiC,T1C
Nは適している。保護膜り5〉に対しては、高温での拡
散が小さいこと、使用温度以上の軟化点あるいは融点で
あること、長地縁体であること。そのため、5i02.
Al2O3等の高軟化点、高融点で安定々カラス質や
八IN、 13N等のセラミソクスが考えられる。例え
ば、5102であれば軟化点1710°Cく水晶)、融
点1470℃〈結晶)、A ]−203であれば融点2
030°Cである。また、Cab、 Y2O3等のよう
に焼成時に外部へ飛散するものを含んだものでもよい。For example, the following properties are required for each material. The insulating member (4) corresponding to the substrate, which is the structure of the electron emitting device, has good thermal conductivity.
Thermal expansion coefficient or heater resistor film <3) and reducing member <2
It is similar to that of 〉, has a long edge, is prone to dielectric breakdown at high temperatures, and is smooth. Therefore, considering availability, 8IN, A1.203, etc. are considered. For the resistor film for heaters (3), the vapor pressure in the high temperature range should be low and the electrical characteristics should be stable in the high temperature range. Therefore, Mo
, W, Pt, TaTiN, TiC, T1CN, etc. can be considered. In particular, TiN, TiC, and T1C, which have a high recrystallization temperature and good stability at high temperatures, have a high recrystallization temperature.
N is suitable. For the protective film 5>, diffusion at high temperatures should be small, the softening point or melting point should be higher than the operating temperature, and the film should have a long edge. Therefore, 5i02.
Possible materials include Al2O3, which has a high softening point and high melting point, and is stable and glassy, and ceramic materials such as 8IN and 13N. For example, 5102 has a softening point of 1710°C (quartz), a melting point of 1470°C (crystalline), and A ]-203 has a melting point of 2
030°C. It may also contain substances that are scattered outside during firing, such as Cab, Y2O3, etc.
還元部材(2)としては、高温域での蒸気圧が低いこと
、高温域での電気特性が安定なこと、電子放射部材<1
)の還元性が高いこと、電子放射部材<1)とのたじみ
の良い多孔質体の膜であること。The reducing member (2) must have low vapor pressure in a high temperature range, stable electrical properties in a high temperature range, and an electron emitting member <1
) has a high reducing property, and the porous membrane has good compatibility with the electron emitting member <1).
ここては、上記条件を鑑み、絶縁部拐り4)としては単
結晶サファイヤ基板〈八1.203)を用い、還元部組
〈2〉としては粉末Wをサファイヤ基板上に焼結させ、
ヒータ用抵抗体膜〈3〉としてTiNをスバ・ツタ法て
形威し、絶縁性の保護膜〈5)として八INをスパッタ
法で形威し、還元部材(2)のWの上に電子放射部材(
1)(Ba、Sr、Ca)CO3を塗布した電子放射装
置の製造方法について述べる。なお、参考写真に実施例
に還元部組(2)として用いた多孔質なW膜の表面写真
を示す。写真中、0067はフィルム番号、 +5.O
KVは走査電子顕微鏡の加速電圧、X2.000は倍率
2000倍、10μmはその直上の線の長さが10μm
に相当することを表す。In view of the above conditions, a single-crystal sapphire substrate (81.203) is used as the insulating part 4), and powder W is sintered on the sapphire substrate as the reducing part 2).
As the heater resistor film <3>, TiN was formed by the sputtering method, and as the insulating protective film <5), 8IN was formed by the sputtering method, and electrons were deposited on the W of the reducing member (2). Radiating member (
1) A method for manufacturing an electron emitting device coated with (Ba, Sr, Ca) CO3 will be described. The reference photograph shows a surface photograph of the porous W film used as the reduction subassembly (2) in the example. In the photo, 0067 is the film number, +5. O
KV is the accelerating voltage of the scanning electron microscope, X2.000 is the magnification of 2000 times, and 10 μm is the length of the line directly above it is 10 μm.
represents that it corresponds to
まず、片面のみ鏡面研磨仕上げを行ったサファイヤ基板
り4〉を用意し、鏡面仕上げではない方の面に所望のカ
ソード用パターンを有機溶媒や焼成助剤を含んだWペー
ストによりスクリーン印刷し、高温(1000〜180
0 °C)で焼成する。カソード側のパターンは比較
的単純であるので鏡面仕上げの面でなくても精度的には
満足できる。次に鏡面仕上げを行った面に所望のヒータ
パターンのマスクを設定し、スパッタ法により所望の厚
さ(数μm〜10μm)のTiN膜(3)を形成する。First, prepare a sapphire substrate 4 with mirror-polished finish on only one side, screen print the desired cathode pattern on the non-mirror-finished surface using W paste containing an organic solvent and baking aid, and then (1000-180
0 °C). Since the pattern on the cathode side is relatively simple, the accuracy can be satisfied even if the surface is not mirror-finished. Next, a mask with a desired heater pattern is set on the mirror-finished surface, and a TiN film (3) of a desired thickness (several μm to 10 μm) is formed by sputtering.
次にヒータパターンの形成された面にスパッタ法により
AIN膜(5〉を形成し、ヒータ用抵抗体膜(3)を似
う。Next, an AIN film (5) is formed by sputtering on the surface on which the heater pattern is formed, and a heater resistor film (3) is formed thereon.
方、還元部材であるW〈2〉表面には電子放射部材〈]
〉、例えば(Bn、 Sr、 Ca)CO3を塗布する
。これにより電子放射装置が完成する。 次に動作に
ついて簡単に説明する。ヒータ用抵抗体膜〈3)に定電
圧を印加し、ヒータ用抵抗体膜〈3〉を所定の温度まで
加熱する。絶縁部拐〈4〉を介して還元部組(2)およ
び電子放射部材(1)を加熱し、グリッド・カソード間
に電圧を印加して、電子放射部材(1)より電子を放射
させる。On the other hand, there is an electron emitting member on the surface of W (2) which is the reducing member.
>, for example, apply (Bn, Sr, Ca)CO3. This completes the electron emitting device. Next, the operation will be briefly explained. A constant voltage is applied to the heater resistor film <3>, and the heater resistor film <3> is heated to a predetermined temperature. The reducing part assembly (2) and the electron emitting member (1) are heated through the insulating part (4), and a voltage is applied between the grid and the cathode to cause the electron emitting member (1) to emit electrons.
こういった電子放射装置の長時間の使用に対して、ヒー
タ用抵抗体膜〈3)は再結晶温度が高く、高温安定性が
良好であるので、抵抗値の変化は小さく、ヒータとして
安定で、また保護膜り5)で覆われているので、例えば
雰囲気中の残留ガスによる腐食の促進等の外部雰囲気に
より損傷を受けることもなく、しかも基板<4〉からの
剥離も防止できる。また、還元部材〈2)は鏡面仕上げ
でない面に焼結して形成したので、付着力が強く高温で
安定であり、しかも多孔質体であるため、一部電子放射
部材<1〉が侵入してくるなど電子放射部材(1)との
なじみが良く、安定して高電流密度が得られる。For long-term use of such electron emitting devices, the heater resistor film (3) has a high recrystallization temperature and good high-temperature stability, so the change in resistance value is small and it is stable as a heater. Also, since it is covered with the protective film 5), it will not be damaged by the external atmosphere, such as acceleration of corrosion due to residual gas in the atmosphere, and it can also be prevented from peeling off from the substrate <4>. In addition, since the reducing member <2) is formed by sintering on a surface that is not mirror-finished, it has strong adhesion and is stable at high temperatures.Moreover, since it is a porous material, some of the electron emitting member <1> may penetrate. It has good compatibility with the electron emitting member (1) such as iron, and a stable high current density can be obtained.
また、大面積の絶縁部材(4)にヒータ、カソードを一
括して形成した後、最小チップに分割して電子放射装置
を、製品間のばらつきが少なく、しかも多量に生産する
ことも可能である。In addition, after forming the heater and cathode all at once on a large-area insulating member (4), it is possible to divide it into the smallest chips to produce an electron emitting device in large quantities with less variation between products. .
なお、ヒータ用抵抗体膜<3)をTiC,TiN。Note that the heater resistor film <3) is TiC or TiN.
T1CNの単体もしくはその混合物で形成する理由は、
再結晶温度が高く、高温での電気的安定性が高いからで
ある。例えば、還元部材〈2〉と同様にWやMO等の一
般的なヒータ材で形成することも考えられる。こういっ
た材料系は1000℃程度の高温で使用している際に基
板であるAl2O3の酸素を奪って(還元して)蒸気圧
の高い酸化物を形成して飛散していく。即ちヒータがエ
ンチングされ、形状が変化してしまう。そのため、ヒー
タとして安定に使用できる環境、例えば基板(4)材、
雰囲気、温度が限定されてしまう。但し、800℃程度
以下ではWやMoも使用可と戒りうる。The reason for forming T1CN alone or a mixture thereof is as follows.
This is because it has a high recrystallization temperature and high electrical stability at high temperatures. For example, like the reducing member <2>, it is also possible to form it from a general heater material such as W or MO. When these materials are used at high temperatures of about 1000° C., they deprive (reduce) oxygen from the substrate Al2O3, form oxides with high vapor pressure, and scatter. In other words, the heater is quenched and its shape changes. Therefore, the environment where it can be used stably as a heater, such as the substrate (4) material,
Atmosphere and temperature are limited. However, it should be noted that W and Mo can also be used at temperatures below about 800°C.
1 また、上記実施例ではヒータ材であるT i C。1 Further, in the above embodiment, T iC is a heater material.
TiN、T1CNをスパッタ法で形成する方法について
述べたが、イオンブレーティングや電子ビーム蒸着、レ
ーザPVD法等のいわゆるPVD法で形成することがで
きることは言うまでもムい。Although the method of forming TiN and T1CN by the sputtering method has been described, it goes without saying that they can also be formed by a so-called PVD method such as ion blasting, electron beam evaporation, or laser PVD method.
また、高温で使用することを考慮すれば、TiCl4、
CH4,N83等を用いた熱CVD法が熱平衡的に
最良と考えられる。また、成膜手法としては同様なガス
を用いたプラズマCVD法もある。In addition, considering the use at high temperatures, TiCl4,
The thermal CVD method using CH4, N83, etc. is considered to be the best in terms of thermal equilibrium. Further, as a film forming method, there is also a plasma CVD method using a similar gas.
また、上記実施例では絶縁部材(4)として単結晶Al
2O3基板を用いたが、リーク電流や絶縁耐圧の条件が
厳しくない場合は、AIN焼結基板及びこれにさらにA
1N膜を底膜したような基板を用いてもよい。Further, in the above embodiment, the insulating member (4) is made of single crystal Al.
A 2O3 substrate was used, but if the leakage current and dielectric strength conditions are not strict, an AIN sintered substrate and an A
A substrate with a 1N film as a bottom film may also be used.
さらに、上記実施例では還元部材り2〉はWペース)・
をスクリーン印刷で形成する方法を用いた例について説
明したが、パターン精度によっては溶射やタラディング
等で形成したものをエツチングしてカソード用パターン
を形成しても良い。Furthermore, in the above embodiment, the reducing member 2> is W pace).
Although an example using a method of forming the cathode pattern by screen printing has been described, depending on the pattern accuracy, the cathode pattern may be formed by etching a pattern formed by thermal spraying, tardding, etc.
[発明の効果]
2
以上のように、この発明によれば、良熱電導性の絶縁部
材、この絶縁部材の一方の面に高融点良電気電導性材料
を用いて所定形状に形成された膜密度の高い緻密な抵抗
体膜、この抵抗体膜を覆うように形成された絶縁性保護
膜、上記絶縁部材の他方の面に良熱電導性還元材料を用
いて所定形状に形成され、上記抵抗体膜より膜密度の低
い多孔質な還元部材、およびこの還元部材上で一部が還
元部材の孔に侵入して形成された電子放射部材を備えた
ので、抵抗体膜は保護膜により外部雰囲気から保護され
ると共に、緻密な抵抗体膜の絶縁部材からの剥離を抑制
し、安定した電子放射装置のヒータを提供でき、さらに
、還元部材を多孔質体で形成することにより、還元部材
上に設けられた電子放射部材とのなじみを良くし、また
電子放射部材の一部が還元部材へ侵入するため、電子放
射の高効率化が実現でき、寿命が長く、高性能で信頼性
の高い電子放射装置を提供することができるという効果
を有する。[Effects of the Invention] 2 As described above, according to the present invention, there is provided an insulating member with good thermal conductivity, and a film formed in a predetermined shape using a high melting point and good electrical conductivity material on one surface of the insulating member. A dense and precise resistor film, an insulating protective film formed to cover the resistor film, and a predetermined shape formed using a good heat conductive reducing material on the other surface of the insulating member, Since the resistor film is equipped with a porous reducing member having a lower film density than the body membrane and an electron emitting member formed on the reducing member by partially penetrating the pores of the reducing member, the resistor film is protected from the external atmosphere by the protective film. In addition, by suppressing the peeling of the dense resistor film from the insulating member, it is possible to provide a stable heater for the electron emitting device.Furthermore, by forming the reducing member with a porous material, the This improves the compatibility with the provided electron emitting member, and a portion of the electron emitting member penetrates into the reducing member, making it possible to achieve high efficiency in electron emission, and to achieve long-life, high-performance, and reliable electron emission. This has the effect of providing a radiation device.
第1図はこの発明の一実施例による電子放射装置を示す
断面構成図、第2図は厚膜回路技術を利用して形成した
従来の電子放射装置を示す断面構成図、第3図は薄膜形
成法による従来の電子放射装置を示す断面構成図である
。
図において、り1)は電子放射部材、(2〉は還元部材
、(3〉はヒータ用抵抗体膜、(4)は絶縁部材。
(5)は保護膜である。
なお、図中同一符号は同一部分または相当部分を示す。FIG. 1 is a cross-sectional configuration diagram showing an electron emission device according to an embodiment of the present invention, FIG. 2 is a cross-sectional configuration diagram showing a conventional electron emission device formed using thick film circuit technology, and FIG. 3 is a thin film circuit diagram. FIG. 2 is a cross-sectional configuration diagram showing a conventional electron emitting device formed by a forming method. In the figure, 1) is an electron emitting member, (2> is a reducing member, (3> is a heater resistor film, (4) is an insulating member, and (5) is a protective film. Note that the same reference numerals are used in the figure. indicates the same or equivalent part.
Claims (1)
融点良電気電導性材料を用いて所定形状に形成された膜
密度の高い緻密な抵抗体膜、この抵抗体膜を覆うように
形成された絶縁性保護膜、上記絶縁部材の他方の面に良
熱電導性還元材料を用いて所定形状に形成され、上記抵
抗体膜より膜密度の低い多孔質な還元部材、およびこの
還元部材上で一部が還元部材の孔に侵入して形成された
電子放射部材を備えた電子放射装置。An insulating member with good thermal conductivity, a dense resistor film formed in a predetermined shape using a high melting point and good electrical conductivity material on one side of this insulating member, and a dense resistor film covering this resistor film. an insulating protective film formed, a porous reducing member formed into a predetermined shape using a good thermally conductive reducing material on the other surface of the insulating member and having a lower film density than the resistor film; and this reducing member. An electron emitting device comprising an electron emitting member formed by partially penetrating into the hole of the reducing member.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1178707A JPH0343932A (en) | 1989-07-10 | 1989-07-10 | Electron emitting apparatus |
| EP90302938A EP0389228B1 (en) | 1989-03-24 | 1990-03-19 | High temperature operating element |
| DE69016235T DE69016235T2 (en) | 1989-03-24 | 1990-03-19 | High temperature component. |
| US07/495,127 US5118983A (en) | 1989-03-24 | 1990-03-19 | Thermionic electron source |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1178707A JPH0343932A (en) | 1989-07-10 | 1989-07-10 | Electron emitting apparatus |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0343932A true JPH0343932A (en) | 1991-02-25 |
Family
ID=16053156
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1178707A Pending JPH0343932A (en) | 1989-03-24 | 1989-07-10 | Electron emitting apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0343932A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6768566B2 (en) | 1998-04-15 | 2004-07-27 | Duke University | Projection screen apparatus including holographic optical element |
-
1989
- 1989-07-10 JP JP1178707A patent/JPH0343932A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6768566B2 (en) | 1998-04-15 | 2004-07-27 | Duke University | Projection screen apparatus including holographic optical element |
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