JPH11118999A - Bi-directional irradiation electron gun and gas-treating device - Google Patents
Bi-directional irradiation electron gun and gas-treating deviceInfo
- Publication number
- JPH11118999A JPH11118999A JP9286763A JP28676397A JPH11118999A JP H11118999 A JPH11118999 A JP H11118999A JP 9286763 A JP9286763 A JP 9286763A JP 28676397 A JP28676397 A JP 28676397A JP H11118999 A JPH11118999 A JP H11118999A
- Authority
- JP
- Japan
- Prior art keywords
- electron
- gas
- electron beam
- electron gun
- vacuum vessel
- 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.)
- Withdrawn
Links
- 238000010894 electron beam technology Methods 0.000 claims abstract description 39
- 239000000463 material Substances 0.000 claims description 18
- 230000002457 bidirectional effect Effects 0.000 claims description 13
- 230000005540 biological transmission Effects 0.000 abstract description 9
- 230000005684 electric field Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 239000012212 insulator Substances 0.000 description 3
- 230000015556 catabolic process Effects 0.000 description 2
- 239000010406 cathode material Substances 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 238000001035 drying Methods 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
Landscapes
- Electron Sources, Ion Sources (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は双方向照射電子銃及
びガス処理装置に関し、特にガス処理装置、フィルム処
理装置、インク乾燥固化装置の電子ビーム反応容器に適
用される電子銃、及びこの電子銃を用いたガス処理装置
に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a bidirectional irradiation electron gun and a gas processing apparatus, and more particularly to an electron gun applied to an electron beam reaction vessel of a gas processing apparatus, a film processing apparatus, an ink drying and solidifying apparatus, and this electron gun. The present invention relates to a gas processing apparatus using the same.
【0002】[0002]
【従来の技術】従来の電子ビームによるガス処理装置は
ガス管外に電子銃を置き、ガス管内のガス全てに電子ビ
ームを照射するために、高電圧で高エネルギーに加速し
た電子ビームを用いていた。このときの電子銃は点電子
源を用いていた。2. Description of the Related Art In a conventional gas processing apparatus using an electron beam, an electron gun is placed outside a gas tube and an electron beam accelerated to a high voltage and high energy is used to irradiate all the gas in the gas tube with the electron beam. Was. At this time, the electron gun used a point electron source.
【0003】図7は、従来の点電子源高電圧電子銃を示
す。図中の付番21は、真空容器である。この真空容器21
の底部側(ガス管22側)には、前記真空容器21の一部を
なす電子ビーム透過窓23が設けられている。前記真空容
器21内には、該容器21の上側から順にヒータ24、電子放
出材料25、ドーナツ状の陽極26、偏向磁石27が夫々配置
されている。前記電子放出材料25はヒータ24により加熱
される。なお、図中の付番28は、電子放出材料25より放
出される電子ビームである。FIG. 7 shows a conventional point electron source high voltage electron gun. Reference number 21 in the figure is a vacuum container. This vacuum vessel 21
An electron beam transmission window 23 which forms a part of the vacuum vessel 21 is provided on the bottom side (on the gas pipe 22 side). In the vacuum vessel 21, a heater 24, an electron-emitting material 25, a donut-shaped anode 26, and a deflecting magnet 27 are arranged in this order from the upper side of the vessel 21. The electron emission material 25 is heated by the heater 24. Reference numeral 28 in the drawing denotes an electron beam emitted from the electron-emitting material 25.
【0004】ところで、図7の点電子源高電圧電子銃の
場合、多くのX線発生があった。X線発生を抑えるには
加速電圧を低くする必要があるが、その場合、大気中で
の電子ビームの飛程が短くなるため、大口径のガス管に
は適用できなかった。これを解決するためには、ガス管
内へのに組み込みが可能な長い直線状陰極型電子銃が適
している。従来はこの様な電子銃がなかった。In the case of the point electron source high voltage electron gun shown in FIG. 7, many X-rays were generated. In order to suppress the generation of X-rays, it is necessary to lower the accelerating voltage. However, in this case, the range of the electron beam in the atmosphere becomes short, so that it cannot be applied to a large-diameter gas pipe. In order to solve this, a long linear cathode type electron gun which can be incorporated into a gas tube is suitable. Conventionally, there was no such an electron gun.
【0005】[0005]
【発明が解決しようとする課題】X線の発生を抑えるに
は電子ビームの加速電圧を低くし、約300KV程度で
ガス等の大気中の対象物に照射する必要がある。このと
き、飛程は70cm程度であるので、直線状電子銃の間
隔は最大70cm程度となり、狭く、直線状電子銃の本
数も多くなる。In order to suppress the generation of X-rays, it is necessary to lower the accelerating voltage of the electron beam and irradiate an object in the atmosphere such as a gas at about 300 KV. At this time, since the range is about 70 cm, the interval between the linear electron guns is about 70 cm at the maximum, which is narrow, and the number of linear electron guns is large.
【0006】本発明はこうした事情を考慮してなされた
もので、円筒形の真空容器の外郭部の2個所に電子ビー
ム透過窓及び陽極を設けるとともに、前記真空容器の中
心線上に前記陽極と対となるように設けた2個の陰極を
有する陰極ユニットを配置した構成とすることにより、
1本の電子銃からガス流れに対して互いに反対方向に2
方向に電子ビームを出すようにし、もってガス管内に組
み込んだ電子銃の間隔を広くして圧力損失を減少させる
とともに、電子銃の本数を半減し、低コスト、小占有面
積の双方向照射電子銃を提供することを目的とする。The present invention has been made in view of such circumstances, and provides an electron beam transmission window and an anode at two locations on the outer periphery of a cylindrical vacuum vessel, and pairs the anode with the anode on the center line of the vacuum vessel. By arranging a cathode unit having two cathodes provided so that
The direction of gas flow from one electron gun
A two-way irradiation electron gun that emits an electron beam in the direction, reduces the pressure loss by widening the interval between the electron guns incorporated in the gas pipe, halves the number of electron guns, and has a low cost and small occupation area. The purpose is to provide.
【0007】本発明は、また被処理ガスの流れを横切る
方向に電子ビームを照射するように前記双方向照射電子
銃を配置してガス処理する構成とすることにより、X線
発生量を抑えつつ大口径のガス管に適用可能なガス処理
装置を提供すること目的とする。According to the present invention, the bidirectional irradiation electron gun is arranged so as to irradiate the electron beam in a direction crossing the flow of the gas to be treated, and the gas treatment is performed. An object of the present invention is to provide a gas processing device applicable to a large-diameter gas pipe.
【0008】[0008]
【課題を解決するための手段】本願第1の発明は、円筒
形の真空容器と、この真空容器の外郭部の2個所に設け
られた電子ビーム透過窓及び陽極と、前記真空容器の中
心線上に配置され、前記陽極と対となるように設けられ
た2個の陰極を有する陰極ユニットとを具備することを
特徴とする双方向照射電子銃である。According to a first aspect of the present invention, there is provided a cylindrical vacuum vessel, an electron beam transmitting window and an anode provided at two positions on the outer periphery of the vacuum vessel, and a center line of the vacuum vessel. And a cathode unit having two cathodes provided so as to be paired with the anode.
【0009】第1の発明において、前記陰極ユニット
は、電子放出材料と、この電子放出材料から発生する電
子ビーム方向に対して67.5°の角度を有する収束電
極を有することが好ましい。In the first invention, it is preferable that the cathode unit has an electron-emitting material and a focusing electrode having an angle of 67.5 ° with respect to a direction of an electron beam generated from the electron-emitting material.
【0010】本願第2の発明は、被処理ガスの流れを横
切る方向に電子ビームを照射するように双方向照射電子
銃を配置してガス処理することを特徴とするガス処理装
置である。A second invention of the present application is a gas processing apparatus characterized in that a gas treatment is performed by disposing a bidirectional irradiation electron gun so as to irradiate an electron beam in a direction crossing the flow of a gas to be treated.
【0011】[0011]
【発明の実施の形態】以下、本発明の一実施例に係る双
方向照射電子銃について、図1を参照して説明する。図
中の付番1は円筒形の真空容器である。この真空容器1
内は、10-7Torr台以下の真空圧力に保たれている。
この真空容器1の外郭部には、真空容器1の一部をなす
電子ビーム透過窓2,3が夫々離間して設けられてい
る。前記電子ビーム透過窓2,3の内側には、夫々棒状
の一対の陽極4,5が互いに平行に設けられている。前
記真空容器1内の略中央部には、前記陽極4,5と対と
なるように設けられた2個の陰極6,7からなる陰極ユ
ニット8が配置されている。ここで、陰極ユニット8は
ほぼダルマ型の断面形状を有している。DESCRIPTION OF THE PREFERRED EMBODIMENTS A bidirectional irradiation electron gun according to one embodiment of the present invention will be described below with reference to FIG. Reference numeral 1 in the figure denotes a cylindrical vacuum vessel. This vacuum vessel 1
The inside is kept at a vacuum pressure of the order of 10 −7 Torr or less.
Electron beam transmission windows 2 and 3 forming a part of the vacuum vessel 1 are provided separately from each other at an outer portion of the vacuum vessel 1. Inside the electron beam transmission windows 2 and 3, a pair of rod-shaped anodes 4 and 5 are provided in parallel with each other. A cathode unit 8 including two cathodes 6 and 7 provided so as to be paired with the anodes 4 and 5 is disposed at a substantially central portion in the vacuum vessel 1. Here, the cathode unit 8 has a substantially Dharma-shaped cross-sectional shape.
【0012】前記陰極ユニット8は、詳しくは図2に示
すような断面形状となっている。即ち、一方の陰極6に
は夫々収束電極61 ,62 が設けられ、他方の陰極7に
は夫々収束電極71 ,72 が設けられている。前記陰極
ユニット8の窪んだ部分(内側寄り)には、電子放出材
料(陰極材料)9が陰極ユニット8の外周10と電気的に
絶縁されて配置されている。ここで、電子放出材料9と
して例えばBaO粉末等を含浸させた陰極材料を用いる
場合、1000〜1100℃に加熱することによって所
定の電流量が得られる。前記電子放出材料9の内側に
は、該材料9を加熱するために2方向それぞれに独立し
てヒータ11が配置されている。電子放出材料9は、主に
ヒータ11からの輻射によって加熱される。前記電子放出
材料9は、陰極外周10に設けられた幅1mm程度の隙間
12から電子ビーム13を放出する。そして、電子放出材料
9と陰極外周10の電位を制御することにより、電子放出
材料9からの電子ビーム電流を調整できる。The cathode unit 8 has a sectional shape as shown in FIG. That is, one cathode 6 is provided with focusing electrodes 6 1 and 6 2 , respectively, and the other cathode 7 is provided with focusing electrodes 7 1 and 7 2 , respectively. An electron-emitting material (cathode material) 9 is disposed in a recessed portion (closer to the inside) of the cathode unit 8 so as to be electrically insulated from the outer periphery 10 of the cathode unit 8. Here, when a cathode material impregnated with, for example, BaO powder or the like is used as the electron-emitting material 9, a predetermined amount of current can be obtained by heating to 1000 to 1100 ° C. Inside the electron emitting material 9, heaters 11 are arranged independently in two directions to heat the material 9. The electron emission material 9 is heated mainly by radiation from the heater 11. The electron emitting material 9 is provided in a gap of about 1 mm width provided on the outer periphery 10 of the cathode.
An electron beam 13 is emitted from 12. Then, by controlling the potentials of the electron emitting material 9 and the cathode outer periphery 10, the electron beam current from the electron emitting material 9 can be adjusted.
【0013】こうした構成の双方向照射電子銃におい
て、前記陰極ユニット8の窪んだ部分から電子ビーム13
が出て、2本の平行な陽極4,5の間を通った後、前記
電子ビーム透過窓2,3を通ってガス中に放出される。
電子ビーム13は対称面14に対称に2方向に放出される。
また、電子ビーム13は正反対の方向ではなく、真空容器
1の中のガス流れの下流方向に対して約67.5°
(θ)の角度で夫々開いている。In the bidirectional irradiation electron gun having such a configuration, the electron beam 13
After passing between the two parallel anodes 4 and 5, is emitted into the gas through the electron beam transmitting windows 2 and 3.
The electron beam 13 is emitted in two directions symmetrically with respect to the plane of symmetry 14.
Also, the electron beam 13 is not in the opposite direction but about 67.5 ° with respect to the downstream direction of the gas flow in the vacuum vessel 1.
Each is open at an angle of (θ).
【0014】これは、図2に示すように、収束電極6
1 ,62 (又は71 ,72 )の角度が電子ビーム13に対
して67.5°となったとき、電子放出材料9から出た
電子ビーム13が電界の作用によって平行に進むことを利
用したものである。つまり、一方の収束電極71 ともう
一方の電子ビーム源の収束電極72 が平行となるように
したとき、夫々の電子ビーム13はガス下流方向に対して
67.5°となる。こうすることによって、ガスの流れ
に対して電子ビーム透過窓2,3が圧力を受けることが
少なく、また電子銃同士の間隔も広く保てバランスがよ
い。This is because, as shown in FIG.
When the angle of 1 , 6 2 (or 7 1 , 7 2 ) becomes 67.5 ° with respect to the electron beam 13, the electron beam 13 emitted from the electron-emitting material 9 travels in parallel by the action of the electric field. It was used. That is, when the focusing electrode 7 2 of one of the focusing electrodes 7 1 Tomo one electron beam source is made parallel, the electron beam 13 of each will be 67.5 ° with respect to the gas downstream direction. By doing so, the electron beam transmission windows 2 and 3 are less likely to receive pressure due to the flow of gas, and the distance between the electron guns is kept wide and the balance is good.
【0015】図3は、前記陰極ユニットの陰極凸部半径
と表面最大電界強度との関係を示す特性図である。陰極
ユニット8の大きさ、特に曲部の曲率半径は陽極4,5
や真空容器1と陰極ユニット8の間にかかる300KV
の電圧に絶縁破壊しないように決める必要がある。経験
的に表面の電界強度が100KV/cm以下であれば絶
縁破壊しにくいので、曲率半径を横軸にとり、縦軸にあ
らゆる表面での最大電界強度を計算し、最高値を求め
た。例えば、真空容器1の内径がφ250mmのとき、
陰極ユニット8の曲率半径rは約25〜35mmで10
0KV/cm以下という条件を満たした。FIG. 3 is a characteristic diagram showing the relationship between the radius of the cathode protrusion of the cathode unit and the maximum electric field intensity on the surface. The size of the cathode unit 8, particularly the radius of curvature of the curved portion, is
Or 300 KV applied between the vacuum vessel 1 and the cathode unit 8
It is necessary to decide so as not to cause dielectric breakdown at the voltage. Empirically, if the electric field strength on the surface is 100 KV / cm or less, dielectric breakdown is unlikely. Therefore, the radius of curvature is plotted on the horizontal axis, and the maximum electric field strength on all surfaces is calculated on the vertical axis, and the maximum value is obtained. For example, when the inner diameter of the vacuum vessel 1 is φ250 mm,
The radius of curvature r of the cathode unit 8 is about 25 to 35 mm and 10
The condition of 0 KV / cm or less was satisfied.
【0016】図4は、曲率半径r=24cmのときの前
記電子銃の一構成である陰極ユニット断面上半分の当電
位面分布を示す。陰極ユニット8が直線状で長いとき、
真空容器1の円筒面では絶縁上支えることが困難である
ので、図5に示すように上下に絶縁碍子14を設け、そこ
からぶら下げ、下で受ける形となる。絶縁碍子14の真空
容器1と離れた側は300KVの負の高電位にあり、大
気中にあるので、大気中で放電しないようコロナリング
15で囲んでいる。そして、コロナリング15から高圧ケー
ブルでヒータ加熱及び陰極ユニット8及び陰極外周10間
の電位制御、高電圧供給を行う。FIG. 4 shows an equipotential surface distribution of the upper half of the cross section of the cathode unit, which is one configuration of the electron gun, when the radius of curvature r is 24 cm. When the cathode unit 8 is linear and long,
Since it is difficult to support the cylindrical surface of the vacuum vessel 1 in terms of insulation, as shown in FIG. 5, insulators 14 are provided on the upper and lower sides, and the insulators 14 are hung therefrom and received below. The side of the insulator 14 away from the vacuum vessel 1 is at a negative high potential of 300 KV and is in the atmosphere, so that corona ring is used to prevent discharge in the atmosphere.
Surrounded by 15. Then, heating of the heater, control of the potential between the cathode unit 8 and the outer periphery of the cathode 10 and supply of a high voltage are performed from the corona ring 15 with a high-voltage cable.
【0017】図6は、図1に示す双方向照射電子銃の配
線図を示す。図6において、ヒータ11にはヒータ電源61
が接続され、電子放出材料9には制御電源62が接続さ
れ、さらに収束電極71 や陽極5には高圧電源63が接続
されている。なお、ヒータ電力は電子銃長さ1mあたり
2〜3KW必要であった。FIG. 6 shows a wiring diagram of the bidirectional irradiation electron gun shown in FIG. In FIG. 6, a heater 11 is connected to a heater power supply 61.
There are connected, to the electron-emitting material 9 is connected controlled power supply 62 has a high-voltage power supply 63 is connected to a further focusing electrode 7 1 and the anode 5. The heater power required 2-3 KW per 1 m of electron gun length.
【0018】しかして、上記実施例に係る双方向照射電
子銃は、1本の電子銃からガス流れに対して互いに反対
方向に2方向に電子ビーム13を出すような構成となって
いるため、ガス管内に組み込んだ電子銃の間隔が広くな
り圧力損失が減少する。また、電子銃の本数が半減す
る。従って、従来の点電子源高電圧電子銃と比べ、コス
ト低減を図るとともに、占有面積を小さくすることがで
きる。However, the bidirectional irradiation electron gun according to the above embodiment is configured to emit the electron beams 13 in two directions opposite to each other with respect to the gas flow from one electron gun. The distance between the electron guns incorporated in the gas pipe is increased, and the pressure loss is reduced. Also, the number of electron guns is halved. Therefore, as compared with the conventional point electron source high voltage electron gun, the cost can be reduced and the occupied area can be reduced.
【0019】更に、こうした構成の双方向照射電子銃
を、被処理ガスの流れを横切る方向に電子ビーム13が照
射するように配置してガス処理を行う構成とすることに
より、従来の点電子源高電圧電子銃を用いたガス処理装
置と比べ、X線発生量を抑え、しかも大口径のガス管に
適用可能なガス処理装置を実現できる。Further, the conventional point electron source is constructed by arranging the bidirectional irradiation electron gun having such a structure so as to irradiate the electron beam 13 in a direction traversing the flow of the gas to be processed. Compared to a gas processing apparatus using a high-voltage electron gun, it is possible to realize a gas processing apparatus that suppresses the amount of X-ray generation and is applicable to a large-diameter gas pipe.
【0020】[0020]
【発明の効果】以上詳述したように本発明によれば、円
筒形の真空容器の外郭部の2個所に電子ビーム透過窓及
び陽極を設けるとともに、前記真空容器の中心線上に前
記陽極と対となるように設けた2個の陰極を有する陰極
ユニットを配置した構成とすることにより、1本の電子
銃からガス流れに対して互いに反対方向に2方向に電子
ビームを出すようにし、もってガス管内に組み込んだ電
子銃の間隔を広くして圧力損失を減少させるとともに、
電子銃の本数を半減で、低コスト、小占有面積の双方向
照射電子銃を提供できる。As described above in detail, according to the present invention, an electron beam transmitting window and an anode are provided at two locations on the outer periphery of a cylindrical vacuum vessel, and the anode and the anode are paired with each other on the center line of the vacuum vessel. A configuration in which a cathode unit having two cathodes provided so as to be arranged is arranged so that an electron beam is emitted from a single electron gun in two directions opposite to each other with respect to a gas flow. In addition to increasing the distance between the electron guns built into the tube to reduce pressure loss,
It is possible to provide a low cost, small occupying area bidirectional irradiation electron gun by halving the number of electron guns.
【0021】また、本発明によれば、被処理ガスの流れ
を横切る方向に電子ビームを照射するように前記双方向
照射電子銃を配置してガス処理する構成とすることによ
り、X線発生量を抑えつつ大口径のガス管に適用可能な
ガス処理装置を提供できる。Further, according to the present invention, the bidirectional irradiation electron gun is arranged so as to irradiate the electron beam in a direction crossing the flow of the gas to be treated, and the gas treatment is performed. It is possible to provide a gas processing apparatus that can be applied to a large-diameter gas pipe while suppressing the occurrence of gas.
【図1】本発明の一実施例に係る双方向照射電子銃の概
略的な全体図。FIG. 1 is a schematic overall view of a bidirectional irradiation electron gun according to an embodiment of the present invention.
【図2】図1の電子銃の一構成である陰極ユニットの断
面図。FIG. 2 is a sectional view of a cathode unit which is one configuration of the electron gun of FIG. 1;
【図3】図2に示す陰極ユニットの陰極凸部半径と表面
最大電界強度との関係を示す特性図。FIG. 3 is a characteristic diagram showing a relationship between a radius of a cathode protrusion and a maximum surface electric field intensity of the cathode unit shown in FIG. 2;
【図4】曲率半径r=24cmのときの図2に示す陰極
ユニット断面上半分の当電位面分布。FIG. 4 is an equipotential surface distribution of the upper half of the cross section of the cathode unit shown in FIG. 2 when the radius of curvature r is 24 cm.
【図5】図1に示す電子銃を組み立てた外観図。FIG. 5 is an external view in which the electron gun shown in FIG. 1 is assembled.
【図6】図1に示す電子銃の配線図。FIG. 6 is a wiring diagram of the electron gun shown in FIG.
【図7】従来の点電子源高電圧電子銃の外観図。FIG. 7 is an external view of a conventional point electron source high voltage electron gun.
【符号の説明】 1…真空容器、 2、3…電子ビーム透過窓、 4、5…陽極、 6、7…陰極、 8…陰極ユニット、 9…電子放出材料、 10…陰極外周、 11…ヒータ、 12…隙間、 13…電子ビーム、 14…対称面。[Description of Signs] 1 ... Vacuum container, 2, 3 ... Electron beam transmission window, 4,5 ... Anode, 6,7 ... Cathode, 8 ... Cathode unit, 9 ... Electron emission material, 10 ... Cathode outer periphery, 11 ... Heater , 12 ... gap, 13 ... electron beam, 14 ... symmetry plane.
Claims (3)
郭部の2個所に設けられた電子ビーム透過窓及び陽極
と、前記真空容器の中心線上に配置され、前記陽極と対
となるように設けられた2個の陰極を有する陰極ユニッ
トとを具備することを特徴とする双方向照射電子銃。1. A vacuum vessel having a cylindrical shape, an electron beam transmitting window and an anode provided at two locations on an outer portion of the vacuum vessel, and arranged on a center line of the vacuum vessel so as to be paired with the anode. And a cathode unit having two cathodes provided for the two-way irradiation electron gun.
この電子放出材料から発生する電子ビーム方向に対して
67.5°の角度を有する収束電極を有することを特徴
とする請求項1記載の双方向照射電子銃。2. The cathode unit, comprising: an electron emission material;
2. The bidirectional irradiation electron gun according to claim 1, further comprising a focusing electrode having an angle of 67.5 [deg.] With respect to a direction of an electron beam generated from the electron emitting material.
ームを照射するように双方向照射電子銃を配置してガス
処理する構成としたことを特徴とする請求項1〜2記載
のガス処理装置。3. The gas processing according to claim 1, wherein a gas is processed by disposing a bidirectional irradiation electron gun so as to irradiate the electron beam in a direction crossing the flow of the gas to be processed. apparatus.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9286763A JPH11118999A (en) | 1997-10-20 | 1997-10-20 | Bi-directional irradiation electron gun and gas-treating device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9286763A JPH11118999A (en) | 1997-10-20 | 1997-10-20 | Bi-directional irradiation electron gun and gas-treating device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH11118999A true JPH11118999A (en) | 1999-04-30 |
Family
ID=17708739
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9286763A Withdrawn JPH11118999A (en) | 1997-10-20 | 1997-10-20 | Bi-directional irradiation electron gun and gas-treating device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH11118999A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102103968A (en) * | 2011-01-19 | 2011-06-22 | 中国科学院近代物理研究所 | Particle beam passable nonmetal vacuum isolation window |
-
1997
- 1997-10-20 JP JP9286763A patent/JPH11118999A/en not_active Withdrawn
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102103968A (en) * | 2011-01-19 | 2011-06-22 | 中国科学院近代物理研究所 | Particle beam passable nonmetal vacuum isolation window |
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