JPS60157148A - Electron generator unit - Google Patents

Electron generator unit

Info

Publication number
JPS60157148A
JPS60157148A JP1255684A JP1255684A JPS60157148A JP S60157148 A JPS60157148 A JP S60157148A JP 1255684 A JP1255684 A JP 1255684A JP 1255684 A JP1255684 A JP 1255684A JP S60157148 A JPS60157148 A JP S60157148A
Authority
JP
Japan
Prior art keywords
pipe
cathode
electron
electron emission
discharge
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
Application number
JP1255684A
Other languages
Japanese (ja)
Inventor
Motoi Obara
基 小原
Kazuo Machida
町田 和雄
Akimichi Nitsuta
新田 晃道
Kanzou Yoshikawa
吉川 皖造
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.)
National Space Development Agency of Japan
Mitsubishi Electric Corp
Original Assignee
National Space Development Agency of Japan
Mitsubishi Electric Corp
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 National Space Development Agency of Japan, Mitsubishi Electric Corp filed Critical National Space Development Agency of Japan
Priority to JP1255684A priority Critical patent/JPS60157148A/en
Publication of JPS60157148A publication Critical patent/JPS60157148A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/02Details
    • H01J37/04Arrangements of electrodes and associated parts for generating or controlling the discharge, e.g. electron-optical arrangement, ion-optical arrangement
    • H01J37/06Electron sources; Electron guns
    • H01J37/077Electron guns using discharge in gases or vapours as electron sources

Abstract

PURPOSE:To reduce discharge holding voltage by forming a gap that is connected to the inner part of an electron emission body between the partial circumference surface of a pipe type electron emission body and the electron emission body holding tool in a hollow cathode type electron generation unit. CONSTITUTION:A cathode disk 4 is arranged so as to be opposed to a keeper electrode 1 and airtightly connected to a cathode pipe 3. Besides, a hollow cathode type electron generation unit is formed by providing a pipe type electron emission body 6 held in the pipe 3 with a holding tool 10 and then a heating heater 7. In this case, the holding tool 10 uses a holding tool 101 so that a gap can be formed by providing a step section (A) on the circumferential surface of the electron emission body 6, and the plasma 12 generated in the cathode pipe 3 can flow in the gap. As a result, since the circumferential surface of the electron emission body 6 can also be used as the electron emission surface, the emission electron amount can be increased and the discharge holding voltage and power consumption can be reduced.

Description

【発明の詳細な説明】 本発明は、中空状の放電陰極(ホローカソード)により
気体放電の効率を高め、かつ該放電により電子を引出す
様にした、電子発生装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electron generating device that uses a hollow discharge cathode to increase the efficiency of gas discharge and extracts electrons through the discharge.

従来より、電子を発生させる装置として、1000℃〜
2500℃に加熱した陰極よりの熱電子放出を利用した
熱電子陰極が最も多用されている。これは構成がシンプ
ルでかつ動作が確実である為である。
Conventionally, as a device that generates electrons, temperatures of 1000℃~
Thermionic cathodes, which utilize thermionic emission from a cathode heated to 2500°C, are most commonly used. This is because the configuration is simple and the operation is reliable.

又、良く収束された細い電子ビームを得る為に電界放出
型の電子銃が利用される事もある。気体放電を利用した
電子銃はプラズマ電子銃とも呼ばれ。
In addition, a field emission type electron gun is sometimes used to obtain a narrow and well-focused electron beam. Electron guns that use gas discharge are also called plasma electron guns.

電子エネルギーの一様性や収束性の面からは、電子ビー
ムとして良質ではないが、高密度の電子ビームが得られ
る為に、電子ビームによる物質の加熱溶解や、イオン源
装置における電子源の様に、ビームの質はあまり問わな
いが大電流を要する様な目的においては良く利用される
Although it is not a high-quality electron beam in terms of electron energy uniformity and convergence, it is possible to obtain a high-density electron beam, so it can be used to heat and melt materials using an electron beam, and as an electron source in an ion source device. In addition, it is often used for purposes that require a large current, although the quality of the beam does not matter much.

ホローカソードはこの様な気体放電を利用した電子源の
一種であって、陰極部をパイプ等により中空状にして、
熱効率を改善した電子源である。
A hollow cathode is a type of electron source that uses gas discharge, and the cathode part is made hollow with a pipe etc.
This is an electron source with improved thermal efficiency.

又該陰極パイプの一部又は全体を仕事関数の低い材料、
いわゆる電子放出材料で構成して、更に効率を改善した
構造も多用される。又、同じ理由により電子放出材料を
陰極パイプ内に挿入する構造も用いられる。第1図は従
来のホローカソード形の電子発生装置の主要部分につい
ての概略構造を表わしている。同図において、(1)は
放電維持用陽極板であって、キーパ−電極とも呼ばれ(
以下キーパ−電極という)%中央に電子引出孔(2)が
あ4(3)は陰極パイプ、(4)は陰極パイプ(3)に
気密接合された陰極円板であって、キーパ−電極(1)
に対向殴中夫に微細孔(5)を穿っている。この微細孔
(5)は、キーパ−電極(1)の電子引出孔(2)とほ
ぼ同軸に配置される。(6)はパイプ状の電子放出体で
あって、保持具aOによって陰極パイプ(3)に保持さ
れている。
In addition, part or all of the cathode pipe is made of a material with a low work function.
Structures made of so-called electron-emitting materials to further improve efficiency are also frequently used. Furthermore, for the same reason, a structure in which an electron-emitting material is inserted into the cathode pipe is also used. FIG. 1 shows a schematic structure of the main parts of a conventional hollow cathode type electron generator. In the figure, (1) is a discharge sustaining anode plate, also called a keeper electrode (
There is an electron extraction hole (2) in the center (hereinafter referred to as keeper electrode), 4 (3) is a cathode pipe, (4) is a cathode disk hermetically sealed to the cathode pipe (3), and the keeper electrode ( 1)
A fine hole (5) was drilled in the husband while he was facing her. This fine hole (5) is arranged approximately coaxially with the electron extraction hole (2) of the keeper electrode (1). (6) is a pipe-shaped electron emitter, which is held on the cathode pipe (3) by a holder aO.

又、保持具αOは適当な支持体(11)により陰極パイ
プ(3)に固定されている。(7)は陰極加熱用ヒータ
ーであって、アrvミ等の耐熱絶縁層(8)により、絶
縁及び保持されている。
Further, the holder αO is fixed to the cathode pipe (3) by a suitable support (11). (7) is a heater for heating the cathode, and is insulated and held by a heat-resistant insulating layer (8) such as an ARv.

次に第2図を参照して、従来のホローカソード形の電子
発生装置の動作について説明する。ホローカソードの起
動にあたってはまず陰極パイプ(3)より放電形成用気
体(9)を導入する。この気体は、陰極円板(4)の微
測オリフィス(5)を通じてキーパ−電極(1)の方に
流机る。次いで、陰極加熱ヒーター(7)に電流を流し
て、陰極パイプ(3)及び陰極円板(4)を加熱すると
共にキーパ−電極(1)に数100vの正の″避圧を印
加する。陰極温度が1000℃前後になると、陰極円板
(4)より発生する熱電子により、陰画円板(4)とキ
ーパ−電極(1)の間に気体放電が発生する。陰極円板
(4)からの熱電子は、放電開始の引き金として作用す
るだけであるからマイクロアンペア程度の電子流で充分
である。放電開始後は以下に述べる様な作用により、パ
イプ状電子放出体(6)とキーパ−電極(1)の間で放
°通が維持される様になり、陰極加熱ヒーター(7)の
通電を中止しても放電が維持される様になる。又当初数
100vあったキーパ−電極(1)の印加電圧は10〜
aOVに低下する。一方キーパー電極(1)の電圧は正
であることから、キーパ−電極(1)に向って電子が流
れ、大部分はキーパ−’At 極(1)に流入するが、
一部はキーパ−電極中央の電子引出孔(2)を11じて
外部に放出される。
Next, referring to FIG. 2, the operation of the conventional hollow cathode type electron generator will be described. To start up the hollow cathode, a discharge forming gas (9) is first introduced from the cathode pipe (3). This gas flows towards the keeper electrode (1) through the micrometering orifice (5) of the cathode disk (4). Next, a current is passed through the cathode heater (7) to heat the cathode pipe (3) and cathode disk (4), and at the same time apply a positive escape pressure of several hundred volts to the keeper electrode (1). When the temperature reaches around 1000°C, gas discharge occurs between the negative disc (4) and the keeper electrode (1) due to thermionic electrons generated from the cathode disc (4). Since the hot electrons only act as a trigger for the start of discharge, an electron flow of about microamperes is sufficient.After the start of discharge, the pipe-shaped electron emitter (6) and the keeper The current is now maintained between the electrodes (1), and even if the cathode heater (7) is no longer energized, the discharge is maintained between the electrodes (1). 1) The applied voltage is 10~
decreases to aOV. On the other hand, since the voltage of the keeper electrode (1) is positive, electrons flow toward the keeper electrode (1), and most of them flow into the keeper electrode (1).
A portion is emitted to the outside through the electron extraction hole (2) in the center of the keeper electrode.

さて次に第2図によりホローカソードの放″醒維持機構
につき説明する。同図においてa力はプラズマである。
Next, the mechanism for maintaining the discharge of the hollow cathode will be explained with reference to Fig. 2. In the figure, the a force is plasma.

一般に持続放電空間においては、通常その空間の大部分
がプラズマで構成される。プラズマ中においては、電子
密度とイオン密度がほぼ等しり、電界はゼロに近い事が
知られている。しかし陰極近傍においては、その電界の
為に電子密度とイオン密度の平衡条件がくずれ、イオン
密度が増大する。又、この平衡部と非平衡部の境界は通
常かなり明確である為、この境界面はプラズマ境界面、
プラズマ境界面と陰極の間はイオンシースと呼ばれ、放
電維持電圧の大部分はイオンシースに掛っている事が知
られている。このイオンシースの厚さは、近似的には、 λn−(EoMTe/e Ine) ”’で表わすこと
が出来る。ここで入口はイオンシースの厚さ%EOは誘
電率、Kはボルツマン係数、Teは電子温度、eは電子
の電荷、n6は電子密度である。
Generally, in a sustained discharge space, most of the space is usually composed of plasma. It is known that in plasma, the electron density and ion density are almost equal, and the electric field is close to zero. However, near the cathode, the electric field disturbs the equilibrium condition between electron density and ion density, and the ion density increases. In addition, since the boundary between this equilibrium part and the non-equilibrium part is usually quite clear, this boundary surface is a plasma boundary surface,
The area between the plasma interface and the cathode is called the ion sheath, and it is known that most of the discharge sustaining voltage is applied to the ion sheath. The thickness of this ion sheath can be approximately expressed as λn-(EoMTe/e Ine) ''.Here, the entrance is the thickness of the ion sheath, %EO is the dielectric constant, K is the Boltzmann coefficient, and Te is the electron temperature, e is the electron charge, and n6 is the electron density.

さて、陰極円板(4)とキーパ−電極(1)の間の放電
で形成されたプラズマは、2λD<<Jの条件が成立す
れば陰極円板(4)の微細孔(5)を通じて、陰極パイ
プ(3)中に入り込み、パイプ状電子放出体(6)の内
筒に到達する事ができる。ここでDiは微細孔(5)の
直径である。パイプ状電子放出体(6)の内表面におい
ては、プラズマ中のイオンによるイオン衝撃により、2
次電子が放出されるが、当該表部の仕事関数が低く、又
、パイプ状電子放出体(6)が陰極パイプ(3)と陰極
円板(4)によって、大略閉じ込められている為にイオ
ン衝撃による加熱の効率が良い、等の条件が重なって電
子放出が活発となる。この結果放電維持電圧が低下する
と共に、陰極ヒーターへの通電を中止しても放電が持続
される様になる。
Now, if the condition of 2λD<<J is satisfied, the plasma formed by the discharge between the cathode disk (4) and the keeper electrode (1) will pass through the micropores (5) of the cathode disk (4). It can enter the cathode pipe (3) and reach the inner cylinder of the pipe-shaped electron emitter (6). Here, Di is the diameter of the micropore (5). On the inner surface of the pipe-shaped electron emitter (6), 2
Secondary electrons are emitted, but because the work function of the surface is low and the pipe-shaped electron emitter (6) is almost confined by the cathode pipe (3) and cathode disk (4), the ions The combination of conditions such as high efficiency of heating by impact leads to active electron emission. As a result, the discharge sustaining voltage decreases, and the discharge continues even if the power supply to the cathode heater is stopped.

さて放電維持電圧はホローカソードの重要な特性値の一
つであって、この電圧を低くおさえる事により、消費電
力が低減するだけでなく、イオンエネルギーが小さくな
るので、イオン衝撃による陰極面の破壊が少くなって、
ホローカソードの寿命を長くする事が出来る。
Now, the discharge sustaining voltage is one of the important characteristic values of the hollow cathode, and by keeping this voltage low, not only the power consumption is reduced, but also the ion energy is reduced, which causes damage to the cathode surface due to ion bombardment. becomes less,
The life of the hollow cathode can be extended.

この様に構成されるホローカソードを用いた電子発生装
置は、キーパ−電圧、すなわち放電維持電圧が低く、従
って消費電力が少く、又かなり長寿命の特性が得られて
いた。しかし、このホローカソード形の電子発生装置を
たとえば宇宙推進機関としてのイオンエンジン等に利用
する様な場合、においては、消費電力及び寿命の点に於
いてなお充分ではない場合が多く、放電維持電圧を更に
低いものにする必要があった。この為発明者らは先に、
第1図におけるパイプ状電子放出体(6)と陰極円板(
4)を密着させず、たとえばα3N程度の間隙をおいて
配置する事により、放電維持電圧が低下する事を発表し
た。
An electron generating device using a hollow cathode constructed in this manner has a low keeper voltage, that is, a discharge sustaining voltage, and thus has low power consumption and a considerably long life. However, when this hollow cathode type electron generator is used, for example, in an ion engine as a space propulsion engine, it is often not sufficient in terms of power consumption and service life, and the discharge maintenance voltage is needed to be lowered even further. For this reason, the inventors first
The pipe-shaped electron emitter (6) and the cathode disk (
It was announced that the discharge sustaining voltage can be lowered by arranging the electrodes 4) with a gap of, for example, α3N, instead of placing them in close contact with each other.

本発明は、これを更に発展させたものであって。The present invention is a further development of this.

パイプ状電子放出体の近傍の形状を工夫する事により、
更に放電維持電圧特性を改善し長寿命でかつ消費電力の
少い電子発生装置を提供する事を目的としたものである
By devising the shape near the pipe-shaped electron emitter,
Furthermore, it is an object of the present invention to provide an electron generator with improved discharge sustaining voltage characteristics, long life, and low power consumption.

以下、本発明の一実施例を第3図に基づいて説明する。Hereinafter, one embodiment of the present invention will be described based on FIG. 3.

同図において(101)は改良された保持具であって、
パイプ状電子放出体(6)の外周表面にあってこれを保
持している。またパイプ状電子放出体(6)の外周表面
に間隙が出来る様に保持具(101)の先端部内面に段
部Aを設けている。その他の構成部分については、第1
図と同様である。
In the figure, (101) is an improved holder,
It is held on the outer peripheral surface of the pipe-shaped electron emitter (6). Further, a stepped portion A is provided on the inner surface of the tip portion of the holder (101) so as to create a gap on the outer circumferential surface of the pipe-shaped electron emitter (6). For other components, please refer to Section 1.
It is similar to the figure.

この様に構成されたこの発明によるホローカソード形の
Y電子発生装置においては、従来技術における場合と同
様に、イオンシースの厚さが、パイプ状電子放出体(6
)の外周面と保持具(101’)の内面との間隙よりも
小さければ、陰極バイブ内のプラズマは該間隙中に浸入
する様になると考えられる。
In the hollow cathode type Y electron generating device according to the present invention configured in this way, the thickness of the ion sheath is the same as in the prior art.
) is smaller than the gap between the outer peripheral surface of the holder (101') and the inner surface of the holder (101'), it is thought that the plasma in the cathode vibe will enter into the gap.

その結果プラズマと電子放出体との対向する面積が増大
して、放出電子量が増加し、かくして放電維持電圧は低
下する。
As a result, the area where the plasma and the electron emitter face each other increases, the amount of emitted electrons increases, and the discharge sustaining voltage decreases.

本発明は、このようにパイプ状電子放出体の外周面をも
、電子放出面として利用できる様工夫したものである。
The present invention is devised so that the outer circumferential surface of the pipe-shaped electron emitter can also be used as an electron emitting surface.

尚、本発明の一実施例の説明においては、保持具の内面
に段差を設けたが、これはもち論、パイプ状電子放出体
(6)の外周面に段差を設けても、同等類似の効果があ
る。又パイプ状電子放出体(6)の保持を電子流の上流
側でのみおこなう様にして、パイプ状電子放出体(6)
と陰極パイプ(3)との間に直接に間隙を作る様にして
も良い。
In the description of one embodiment of the present invention, a step is provided on the inner surface of the holder, but it goes without saying that even if a step is provided on the outer circumferential surface of the pipe-shaped electron emitter (6), the same or similar effective. In addition, the pipe-shaped electron emitter (6) is held only on the upstream side of the electron flow, so that the pipe-shaped electron emitter (6)
A gap may be created directly between the cathode pipe (3) and the cathode pipe (3).

以上の様に本発明においては、パイプ状″ゼ子放出体の
外周面をも゛電子放出面として利用するようにしたので
、放電維持電圧が低下し、この結果消費電力が低減され
、又、イオンエネルギーが下がる為、イオン衝撃による
陰極面の破壊が少くなって、ホローカソードの長寿命化
を計る事ができる。
As described above, in the present invention, the outer peripheral surface of the pipe-shaped "zeon emitter" is used as an electron emitting surface, so that the discharge sustaining voltage is reduced, and as a result, power consumption is reduced. Since the ion energy is lowered, the damage to the cathode surface due to ion bombardment is reduced, and the life of the hollow cathode can be extended.

又電子放出面の拡大は電子放出面の電流密度が下がる事
を意味するので、この結果としても、寿命特性に改善を
はかる事ができる。
Furthermore, since the enlargement of the electron emitting surface means that the current density on the electron emitting surface is reduced, the life characteristics can also be improved as a result.

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

第1図は従来の装置の主要部の断面図、第2図はその動
作説明図、第3図はこの発明の一実施例による装置の主
要部の断面図である。 (1)・・・キーパ−電極、(2)・・・電子放出窓、
(3)・・・陰極パイプ、(4)・・・陰極円板、(5
)・・・微細孔、(6)・・・パイプ状電子放出体、(
7)・・・陰極加熱ヒータ、(8)・・・絶縁層(9)
・・・気体、 01・・・保持具、(1013・・・保
持具%(11)・・・支持体、0■・・・プラズマ 尚1図中同一符号は夫々間−又は相当部分を示す。 代理人大岩増雄
FIG. 1 is a sectional view of the main part of a conventional device, FIG. 2 is an explanatory diagram of its operation, and FIG. 3 is a sectional view of the main part of a device according to an embodiment of the present invention. (1)...Keeper electrode, (2)...Electron emission window,
(3)... Cathode pipe, (4)... Cathode disk, (5
)...Micropore, (6)...Pipe-shaped electron emitter, (
7)...Cathode heater, (8)...Insulating layer (9)
...Gas, 01...Holder, (1013...Holder % (11)...Support, 0■...Plasma In addition, the same symbols in the figure indicate the space or corresponding part, respectively. . Agent Masuo Oiwa

Claims (2)

【特許請求の範囲】[Claims] (1)中央に電子放出孔を有し放電維持用陽極として作
用するキーパ−電極と、このキーパ−電極に対向し、前
記電子放出孔と大略同軸の位置に配置された陰極パイプ
と、この陰極パイプに気密接合され、中央部に微細孔を
有する陰極円板と、この陰極円板近傍の上・記陰極パイ
プ中に挿入されたパイプ状電子放出体と、このパイプ状
電子放出体を保持する保持具と、上記陰極パイプ中に放
電形成用気体を供給し得る機構とを備え、前記隅板円板
と前記パイプ状電子放出体とで構成される陰極部と前記
キーパ−電極との間で、持続気体放電を形成する事によ
り、前記電子放出孔より電子を引出す様にしたホローカ
ソード形の電子発生装置に於いて、前記パイプ状電子放
出体の少なくとも一部の外周面と前記保持具との間に、
前記パイプ状電子放出体の内部に通じる間隙を形成した
事を特徴とする電子発生装置。
(1) A keeper electrode that has an electron emission hole in the center and acts as an anode for sustaining the discharge, a cathode pipe that faces the keeper electrode and is placed approximately coaxially with the electron emission hole, and this cathode. A cathode disk that is hermetically sealed to the pipe and has a fine hole in the center, a pipe-shaped electron emitter inserted into the above cathode pipe near the cathode disk, and a pipe-shaped electron emitter that holds the pipe. a holder, and a mechanism capable of supplying discharge forming gas into the cathode pipe, between the cathode part composed of the corner plate disk and the pipe-shaped electron emitter and the keeper electrode. , in a hollow cathode type electron generating device configured to draw out electrons from the electron emitting hole by forming a sustained gas discharge, the outer circumferential surface of at least a part of the pipe-shaped electron emitting body and the holder; Between,
An electron generating device characterized in that a gap communicating with the inside of the pipe-shaped electron emitter is formed.
(2)間隙はパイプ状電子放出体の陰極円板近傍側に形
成された事を特徴とする特許請求の範囲第1項記載の電
子発生装置。
(2) The electron generating device according to claim 1, wherein the gap is formed on the side near the cathode disk of the pipe-shaped electron emitter.
JP1255684A 1984-01-26 1984-01-26 Electron generator unit Pending JPS60157148A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1255684A JPS60157148A (en) 1984-01-26 1984-01-26 Electron generator unit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1255684A JPS60157148A (en) 1984-01-26 1984-01-26 Electron generator unit

Publications (1)

Publication Number Publication Date
JPS60157148A true JPS60157148A (en) 1985-08-17

Family

ID=11808612

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1255684A Pending JPS60157148A (en) 1984-01-26 1984-01-26 Electron generator unit

Country Status (1)

Country Link
JP (1) JPS60157148A (en)

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