JPH04137441A - High-frequency cavity type electron gun - Google Patents
High-frequency cavity type electron gunInfo
- Publication number
- JPH04137441A JPH04137441A JP2259381A JP25938190A JPH04137441A JP H04137441 A JPH04137441 A JP H04137441A JP 2259381 A JP2259381 A JP 2259381A JP 25938190 A JP25938190 A JP 25938190A JP H04137441 A JPH04137441 A JP H04137441A
- Authority
- JP
- Japan
- Prior art keywords
- frequency
- energy
- electron gun
- electron
- cavity resonator
- 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.)
- Granted
Links
- 230000005684 electric field Effects 0.000 claims description 9
- 238000010894 electron beam technology Methods 0.000 abstract description 7
- 230000007246 mechanism Effects 0.000 abstract description 6
- 238000010586 diagram Methods 0.000 description 7
- 238000000034 method Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 241001270131 Agaricus moelleri Species 0.000 description 1
- 230000001133 acceleration Effects 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
Landscapes
- Particle Accelerators (AREA)
- Electron Sources, Ion Sources (AREA)
Abstract
Description
【発明の詳細な説明】
a、産業上の利用分野
本発明は高周波空胴型電子銃に関するもので、特に高周
波空胴共振器を利用した電子銃に関する。DETAILED DESCRIPTION OF THE INVENTION a. Field of Industrial Application The present invention relates to a high frequency cavity type electron gun, and particularly to an electron gun using a high frequency cavity resonator.
b、従来の技術
一般に、電子ビームを発生させる装置(以下、電子銃と
いう)では、直流電圧を使用した静電型電子銃が用いら
れることが多い。すなわち、電界により電子を放射する
陰極には、例えば先端が約10on−の曲率半径をもっ
た針状タングステンが用いられ、対向する陽極との間に
数kVの電圧を印加して、強電界(>10’V/C11
)にすることにより電子放射させている。b. Prior Art Generally, in devices that generate electron beams (hereinafter referred to as electron guns), electrostatic electron guns that use DC voltage are often used. That is, for example, a needle-shaped tungsten whose tip has a radius of curvature of about 10 on- is used as the cathode that emits electrons by an electric field, and a voltage of several kV is applied between it and the opposing anode to generate a strong electric field ( >10'V/C11
) to emit electrons.
そして、放射電子の一部は更に多段の陽極により所要の
エネルギーにまで加速している。A part of the emitted electrons is further accelerated to the required energy by a multi-stage anode.
しかし、近年ではこれに変わり、高周波電界を用いて電
子を放射させる高周波空胴型電子銃が、利用される機会
が増えてきている。この方法を用いると、小型の本体で
高いエネルギーの電子を発生させることができ、かつ電
子をさらに加速する場合に電子をパンチングする必要が
ない、という利点がある。However, in recent years, this has been replaced by a high-frequency cavity electron gun, which emits electrons using a high-frequency electric field, and has been increasingly used. This method has the advantage that high-energy electrons can be generated with a small body and that there is no need to punch the electrons when further accelerating them.
C0発明が解決しようとする課題
しかしながら、この方法によると発生した電子のエネル
ギーは、第4図に示すように、時間に対して正弦波分布
をもつため、加速器に入射する際に磁場などを用いて、
必要なエネルギーの電子だけを取り出す必要があり、こ
のとき振り分けられた他の電子は電力損失になるという
問題点がある。Problems to be solved by the C0 invention However, as shown in Figure 4, the energy of the electrons generated by this method has a sinusoidal distribution over time, so it is difficult to use a magnetic field etc. when entering the accelerator. hand,
There is a problem in that it is necessary to extract only the electrons with the necessary energy, and the other electrons distributed at this time result in power loss.
また、近年は加速器の開発も進み、加速用の高周波電界
に第三次高調波を混ぜて、電子を加速するための電界を
、多くの時間にわたって均一にした、所謂フラットトッ
プ型の高周波型加速器も建設されているが、従来の高周
波空胴型電子銃では十分にこの装置の能力を引きだせな
かった。In addition, in recent years, the development of accelerators has progressed, and so-called flat-top high-frequency accelerators mix third-order harmonics with the high-frequency electric field for acceleration, making the electric field uniform over a large period of time to accelerate electrons. has been constructed, but conventional high-frequency cavity electron guns were not able to bring out the full potential of this device.
本発明にかかる点に鑑みなされたもので、その目的は前
記問題点を解消し、ある特定のエネルギーの含有率の多
い電子ビームが得られる高周波空胴型電子銃を提供する
ことにある。The present invention has been made in view of the above-mentioned problems, and its purpose is to provide a high-frequency cavity electron gun that can provide an electron beam with a high content of a certain specific energy.
69課題を解決するための手段
前記目的を達成するための本発明の構成は、高周波空胴
共振器の内部に、電界により電子放射する陰極を配設し
た高周波空胴型電子銃において、前記空胴共振器が基本
周波およびその第三次高調波の双方で共振するように形
成されたことを特徴とする。69 Means for Solving the Problems The structure of the present invention for achieving the above-mentioned object is a high-frequency cavity electron gun in which a cathode that emits electrons by an electric field is disposed inside a high-frequency cavity resonator. It is characterized in that the body resonator is formed to resonate at both the fundamental frequency and its third harmonic.
81作用
本発明は以上のように構成されているので、この高周波
空胴型電子銃は基本周波とその第三次高調波の両方で励
振される。81 Effect Since the present invention is constructed as described above, this high frequency cavity electron gun is excited by both the fundamental frequency and its third harmonic.
本発明の試験結果を、従来のものとの比較において説明
する。まず、従来の高周波空胴型電子銃により発生した
電子のエネルギーは、第4図に示すように、時間に対し
て正弦波分布をもっている。すなわち、ある一定の範囲
のエネルギーをもった電子が、全体に占める割合は非常
に少なく、例えば±1%の誤差内のエネルギーをもった
電子は、最も多いものでも全体の6.4%に達しない。Test results of the present invention will be explained in comparison with conventional ones. First, the energy of electrons generated by a conventional high-frequency cavity electron gun has a sinusoidal distribution with respect to time, as shown in FIG. In other words, the proportion of electrons with energy within a certain range is extremely small; for example, the electrons with energies within ±1% of the total account for 6.4% of the total. do not.
しかし、基本周波に適度な割合でその第三次高調波を加
えることによって、電子のエネルギーを、第3図に示す
ように、分布させることも可能であり、この場合±1%
の誤差内のエネルギーをもった電子は、最も多いもので
は全体の15%にも達する。However, by adding the third harmonic to the fundamental frequency at an appropriate rate, it is possible to distribute the electron energy as shown in Figure 3, in which case it is ±1%.
The largest number of electrons with energy within the error range is 15% of the total.
f、実施例
以下、図面に基づいて本発明の好適な実施例を例示的に
詳しく説明する。f. Examples Hereinafter, preferred embodiments of the present invention will be described in detail by way of example based on the drawings.
第1図は本発明の一実施例を示す高周波空胴型電子銃の
構成図、第2図は高周波空胴共振器の概略断面図である
。同図において、1は高周波空胴型電子銃、2は空胴共
振器、3は電子放射用の陰極部、4は先端が針状の陰極
、5,6は空胴共振器2の共振周波数を調整するための
同調機構(または共振周波数可変機構)で、5は基本周
波、6はその第三次高調波をそれぞれ可変できる部分に
配設されている。FIG. 1 is a block diagram of a high frequency cavity type electron gun showing one embodiment of the present invention, and FIG. 2 is a schematic sectional view of a high frequency cavity resonator. In the figure, 1 is a high-frequency cavity electron gun, 2 is a cavity resonator, 3 is a cathode part for electron emission, 4 is a cathode with a needle-like tip, and 5 and 6 are the resonance frequencies of the cavity resonator 2. A tuning mechanism (or resonant frequency variable mechanism) for adjusting the resonance frequency, numeral 5 is a fundamental frequency, and numeral 6 is a part that can vary the third harmonic thereof.
7.8はそれぞれ基本周波およびその第三次高調波の整
合機構で、独立に調整可能であり、9.10はそれぞれ
基本周波およびその第三次高調波を出力する高周波発生
器、11は陰極部3.高周波発生器9,10を動作させ
るための電源装置である。7.8 is a matching mechanism for the fundamental frequency and its third harmonic, which can be adjusted independently, 9.10 is a high frequency generator that outputs the fundamental frequency and its third harmonic, respectively, and 11 is a cathode. Part 3. This is a power supply device for operating the high frequency generators 9 and 10.
空胴共振器2は基本周波に対してT M o r。モー
ドの円筒型共振空胴であるが、通常の形状では第三次高
調波に共振しないので、第2図に示すように、縁2aの
形状によりインピーダンスを変えて丁度3倍の比を持つ
2つの周波数で共振するように形成している。そして、
前記空胴共振器2を共振基本周波(TM、、、モード)
および第三次高調波(TMozoモード)でそれぞれに
励振し、各電力1位相を調整して共振器2の半径方向中
央部の電界が最大部で時間的に極力平坦な特性20を持
つよう調整する。この状態で、陰極4より電子を発生し
高周波電界を利用して電子ビームを取り出すもので、1
2は発生した電子流の経路を示す。The cavity resonator 2 has T M or with respect to the fundamental frequency. The mode is a cylindrical resonant cavity, but the normal shape does not resonate with the third harmonic, so as shown in Figure 2, the impedance is changed depending on the shape of the edge 2a, and the two It is designed to resonate at one frequency. and,
The cavity resonator 2 has a resonant fundamental frequency (TM, mode).
and third harmonic (TMozo mode), and adjust each power 1 phase so that the electric field at the radial center of the resonator 2 has a characteristic 20 that is as flat as possible in time at its maximum. do. In this state, electrons are generated from the cathode 4 and an electron beam is extracted using a high frequency electric field.
2 shows the path of the generated electron flow.
第3図はこの状態における前記空胴共振器2からの放射
電子のエネルギーEの時間Tに対する分布図を示し、第
4図の従来のものによる場合の分布図と比較すると、平
坦な特性部分20を占める割合が多く、ある特定のエネ
ルギーの含有率が多い電子流を得ることができる。FIG. 3 shows a distribution diagram of the energy E of the emitted electrons from the cavity resonator 2 with respect to time T in this state, and when compared with the distribution diagram of the conventional one shown in FIG. It is possible to obtain an electron flow with a high content of a certain energy.
なお、前記空胴共振器2の前記同調機構5,6は、2つ
のモードの共振周波数をそれぞれに微調整できるように
、できるだけ他モードの周波数に影響を及ぼさない一実
施例に設けるのが望ましい。Note that the tuning mechanisms 5 and 6 of the cavity resonator 2 are preferably provided in an embodiment that does not affect the frequencies of other modes as much as possible so that the resonance frequencies of the two modes can be finely adjusted respectively. .
なお、本発明の技術は前記実施例における技術に限定さ
れるものではなく、同様な機能を果す他の態様の手段に
よってもよ(、また本発明の技術は前記構成の範囲内に
おいて種々の変更、付加が可能である。Note that the technology of the present invention is not limited to the technology in the above-mentioned embodiments, but may also be implemented by means of other modes that achieve the same function (also, the technology of the present invention may be modified in various ways within the scope of the above-mentioned configuration). , can be added.
g0発明の効果
以上の説明から明らかなように本発明の高周波空胴型電
子銃によれば、空胴共振器を、基本周波とその第三次高
調波との双方で共振するように形成したので、ある特定
のエネルギーの含有率の多い電子ビームを得ることが可
能となる。g0 Effects of the Invention As is clear from the above explanation, according to the high frequency cavity electron gun of the present invention, the cavity resonator is formed to resonate at both the fundamental frequency and its third harmonic. Therefore, it is possible to obtain an electron beam with a high content of a certain specific energy.
また、本発明は電子のエネルギーの均一性を要求される
技術、例えば電子線直射型の物性加工における加工効率
の向上等にとって、極めて有用である。Further, the present invention is extremely useful for techniques that require uniformity of electron energy, such as improving processing efficiency in physical property processing using direct electron beam radiation.
第1図は本発明の一実施例を示す高周波空胴型電子銃の
構成図、第2図は空胴共振器の概略断面図、第3図は本
実施例による放射電子のエネルギーの時間に対する分布
図、第4図は従来の空胴共振器による放射電子のエネル
ギーの時間に対する分布図である。
1・・・高周波空胴型電子銃、
2・・・空胴共振器、
4・・・陰極、
9・・・高周波(基本周波)発生器、
lO・・・高周波(第三次高調波)発生器。
第
図
/1
第
図FIG. 1 is a block diagram of a high-frequency cavity electron gun showing an embodiment of the present invention, FIG. 2 is a schematic cross-sectional view of a cavity resonator, and FIG. 3 is a diagram showing the energy of emitted electrons according to this embodiment versus time. Distribution diagram, FIG. 4 is a distribution diagram of the energy of emitted electrons by a conventional cavity resonator versus time. DESCRIPTION OF SYMBOLS 1... High frequency cavity electron gun, 2... Cavity resonator, 4... Cathode, 9... High frequency (fundamental frequency) generator, lO... High frequency (third harmonic) generator. Figure/1 Figure
Claims (1)
極を配設した電子銃において、 前記空胴共振器が基本周波およびその第三次高調波の双
方で共振するように形成されたことを特徴とする高周波
空胴型電子銃。[Claims] In an electron gun in which a cathode that emits electrons by an electric field is disposed inside a high-frequency cavity resonator, the cavity resonator resonates at both the fundamental frequency and its third harmonic. A high frequency cavity type electron gun characterized by being formed.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2259381A JP2983272B2 (en) | 1990-09-28 | 1990-09-28 | High frequency cavity type electron gun |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2259381A JP2983272B2 (en) | 1990-09-28 | 1990-09-28 | High frequency cavity type electron gun |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH04137441A true JPH04137441A (en) | 1992-05-12 |
JP2983272B2 JP2983272B2 (en) | 1999-11-29 |
Family
ID=17333344
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2259381A Expired - Lifetime JP2983272B2 (en) | 1990-09-28 | 1990-09-28 | High frequency cavity type electron gun |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2983272B2 (en) |
-
1990
- 1990-09-28 JP JP2259381A patent/JP2983272B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JP2983272B2 (en) | 1999-11-29 |
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