JPH0521824Y2 - - Google Patents
Info
- Publication number
- JPH0521824Y2 JPH0521824Y2 JP3154787U JP3154787U JPH0521824Y2 JP H0521824 Y2 JPH0521824 Y2 JP H0521824Y2 JP 3154787 U JP3154787 U JP 3154787U JP 3154787 U JP3154787 U JP 3154787U JP H0521824 Y2 JPH0521824 Y2 JP H0521824Y2
- Authority
- JP
- Japan
- Prior art keywords
- charged particle
- particle beam
- electrodes
- insulator
- cylindrical 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.)
- Expired - Lifetime
Links
- 239000002245 particle Substances 0.000 claims description 21
- 238000005192 partition Methods 0.000 claims description 14
- 239000000463 material Substances 0.000 claims description 13
- 239000012212 insulator Substances 0.000 description 25
- 238000010894 electron beam technology Methods 0.000 description 12
- 238000003466 welding Methods 0.000 description 4
- 239000002184 metal Substances 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 238000010884 ion-beam technique Methods 0.000 description 2
- 238000007789 sealing Methods 0.000 description 2
- 230000001133 acceleration Effects 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 238000002164 ion-beam lithography Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
Landscapes
- Electron Sources, Ion Sources (AREA)
Description
【考案の詳細な説明】
[産業上の利用分野]
本考案は電子線やイオンビーム等の荷電粒子線
を用いた顕微鏡や描画装置に利用して最適な荷電
粒子線装置に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a charged particle beam device that is most suitable for use in a microscope or drawing device that uses a charged particle beam such as an electron beam or an ion beam.
[従来の技術]
電子顕微鏡やイオンビーム描画装置等の荷電粒
子線装置では、荷電粒子線発生源からの荷電粒子
線を加速し、試料や材料等のターゲツトに照射し
ている。第2図は電子線装置における電子線の加
速部を示しており、1は電子発生陰極、2はウエ
ーネルト電極、3は接地電位の陽極である。該陰
極1と陽極3の間には、高圧電源4によつて加速
電圧が印加されている。5は円筒状の絶縁碍子で
あり、該碍子5の一端は陽極3に固定され、他端
は該陰極と同電位の電極7に固定されており、該
碍子に囲まれた領域は高真空に排気されている。
このような構成において、陰極1から発生した電
子は陽極3によつて加速され、該陽極3の開口を
通過した電子線が該陽極下方に配置されたターゲ
ツトに照射される。[Prior Art] In a charged particle beam device such as an electron microscope or an ion beam lithography device, a charged particle beam from a charged particle beam generation source is accelerated and irradiated onto a target such as a sample or a material. FIG. 2 shows an electron beam accelerating section in an electron beam device, in which 1 is an electron generating cathode, 2 is a Wehnelt electrode, and 3 is an anode at ground potential. An accelerating voltage is applied between the cathode 1 and the anode 3 by a high voltage power supply 4. 5 is a cylindrical insulator; one end of the insulator 5 is fixed to the anode 3, the other end is fixed to the electrode 7 having the same potential as the cathode, and the area surrounded by the insulator is placed in a high vacuum. It is being exhausted.
In such a configuration, electrons generated from the cathode 1 are accelerated by the anode 3, and the electron beam passing through the opening of the anode 3 is irradiated onto a target placed below the anode.
[考案が解決しようとする問題点]
ところで、陽極3に向けて加速された電子線は
その一部が該陽極3の開口を通過するものの、そ
の多くは該陽極に衝突する。この陽極への電子線
の衝突により、該陽極からは加速された入射電子
線と同程度のエネルギーを有する反射電子が発生
する。この反射電子はあらゆる方向に放射し、そ
の結果、絶縁碍子5に向かつた反射電子はそこに
衝突して蓄積され、該碍子表面が帯電することに
なる。該碍子表面の帯電により、該碍子表面の電
位分布が変化し、この変化部で微小放電が発生す
る。この微小放電は陰極1と陽極3との間の碍子
表面を伝わつての沿面放電のトリガとなつてしま
う。[Problems to be Solved by the Invention] Incidentally, although part of the electron beam accelerated toward the anode 3 passes through the opening of the anode 3, most of it collides with the anode. As the electron beam collides with the anode, reflected electrons having energy comparable to that of the accelerated incident electron beam are generated from the anode. The reflected electrons radiate in all directions, and as a result, the reflected electrons directed toward the insulator 5 collide with and accumulate there, causing the surface of the insulator to be charged. Due to the charging of the surface of the insulator, the potential distribution on the surface of the insulator changes, and a micro discharge occurs at this changed portion. This minute discharge triggers a creeping discharge that travels along the insulator surface between the cathode 1 and the anode 3.
そのため、第3図に示すように、絶縁碍子5の
表面部分に高抵抗物質をコーテイングすることが
考えられた。この場合、碍子5に向う反射電子
は、該碍子表面の高抵抗物質を伝わつて直ちに放
電されるので、該碍子の帯電はなくなり、碍子表
面部分での沿面放電を防止することが可能とな
る。しかしながら、該絶縁碍子は、真空隔壁とし
ての役割も担つているため、該碍子5と電極3,
7との間には、真空漏れが生じないように、溶接
を行わねばならない。この絶縁碍子と電極との真
空封じのための溶接は、かなりの高温下で行う必
要があり、その結果、溶接時の高い温度のため、
電極金属がコーテイングされた高抵抗物質中に拡
散してしまい、特に、碍子両端部の電極3,7に
近い部分で、該高抵抗物質の抵抗値が著しく低下
する。従つて、高抵抗物質は、製作時の高い抵抗
値を維持することができず、沿面放電が発生する
以前に電極3と7との間が短絡に近い状態とな
り、高電圧を該電極間に印加することができなく
なつてしまう。又、隔壁部材としての絶縁碍子5
全体を高抵抗物質とした場合にも、真空封じのた
めの高温下での溶接のため、前記と同様に、抵抗
値の低下が生じる。 Therefore, as shown in FIG. 3, it has been considered to coat the surface portion of the insulator 5 with a high-resistance material. In this case, the reflected electrons directed toward the insulator 5 are immediately discharged through the high-resistance material on the surface of the insulator, so that the insulator is no longer charged, making it possible to prevent creeping discharge on the surface of the insulator. However, since the insulator also plays a role as a vacuum partition, the insulator 5 and the electrode 3,
7 must be welded to prevent vacuum leakage. Welding for vacuum sealing between the insulator and the electrode must be performed at a considerably high temperature, and as a result, due to the high temperature during welding,
The electrode metal will diffuse into the coated high-resistance material, and the resistance value of the high-resistance material will drop significantly, especially in the portions near the electrodes 3 and 7 at both ends of the insulator. Therefore, the high-resistance material is unable to maintain a high resistance value during manufacture, and before creeping discharge occurs, electrodes 3 and 7 become almost short-circuited, causing a high voltage to be applied between the electrodes. It becomes impossible to apply any voltage. Moreover, the insulator 5 as a partition wall member
Even when the entire structure is made of a high-resistance material, the resistance value decreases in the same manner as described above because welding is performed under high temperature for vacuum sealing.
本考案は上述した点に鑑みてなされたもので、
沿面放電の発生を防止することができる荷電粒子
線装置を提供することを目的としている。 This invention was made in view of the above points,
It is an object of the present invention to provide a charged particle beam device that can prevent creeping discharge from occurring.
[問題点を解決するための手段]
本考案に基づく荷電粒子線装置は、第1と第2
の電極と、該両電極の間に高電圧を印加する手段
と、該第1と第2の電極の間の荷電粒子線通路の
周囲に配置される隔壁部材とを有し、該電極間で
荷電粒子線を加速あるいは集束させるように構成
した荷電粒子線装置において、該隔壁部材の内側
に、該隔壁部材から離間して、高抵抗物質によつ
て形成された筒状部材を配置し、該筒状部材と該
両電極とを電気的に接続させたことを特徴として
いる。[Means for solving the problem] The charged particle beam device based on the present invention has a first and a second
a means for applying a high voltage between the two electrodes, and a partition member disposed around the charged particle beam passage between the first and second electrodes, In a charged particle beam device configured to accelerate or focus a charged particle beam, a cylindrical member made of a high-resistance material is disposed inside the partition member, spaced apart from the partition member, and It is characterized in that the cylindrical member and both electrodes are electrically connected.
[作用]
第1の電極と第2の電極の間で加速された荷電
粒子線は、該第2の電極に衝突し、反射電子を発
生する。該発生した反射電子は各方向に放射され
るが、両電極の間の荷電粒子線の通路の周囲に配
置される絶縁性の隔壁部材の内側には、高抵抗物
質によつて形成された筒状部材が配置されている
ので、該隔壁部材に向う荷電粒子線は該筒状部材
に衝突し、その表面部分を伝わつて放電され、そ
の結果、該隔壁部材表面の沿面放電を防止するこ
とができる。[Operation] The charged particle beam accelerated between the first electrode and the second electrode collides with the second electrode to generate reflected electrons. The generated backscattered electrons are emitted in each direction, but inside the insulating partition member placed around the path of the charged particle beam between the two electrodes, there is a cylinder made of a high-resistance material. Since the cylindrical member is arranged, the charged particle beam directed towards the partition member collides with the cylindrical member and is transmitted along the surface portion of the cylindrical member to be discharged. As a result, creeping discharge on the surface of the partition member can be prevented. can.
[実施例]
以下本考案の一実施例を添附図面に基づいて詳
述する。[Embodiment] An embodiment of the present invention will be described below in detail based on the accompanying drawings.
第1図は本考案を実施した電子線装置を示して
いるが、第2図、第3図と同一部分は同一番号を
付してその説明を省略する。該第1図に示した装
置の第2図の従来装置と相異する点は、真空隔壁
部材としての絶縁碍子5の内側に、高抵抗物質で
形成された筒状部材8を配置した点である。該筒
状部材は陽極3と電極7に溶接によつて固定され
ており、該部材8と両電極3,7は電気的に接続
される。このように構成したので、該陽極3に、
加速された電子線が衝突することにより発生した
反射電子が該碍子5方向に向つても、該反射電子
は筒状部材8に衝突し、高抵抗物質である筒状部
材を伝わつて直ちに放電されるので、該碍子の帯
電はなくなり、碍子表面部分での沿面放電を完全
に防止することができる。又、真空隔壁としての
役割は絶縁碍子5に担わせており、該筒状部材8
を電極に固定する際には、真空漏れを考慮する必
要がないので、固定に際しては、単に筒状部材8
の両端が電極金属に接するようにすれば良く、電
極金属の該筒状部材への拡散は全く起こらない。
従つて、該筒状部材8の抵抗値は、該部材を製作
したときの値を維持することができる。なお、該
筒状部材8の一部には孔9が穿たれており、該筒
状部材8と絶縁碍子5との間の空間の排気コンダ
クタンスを高めるようにしている。 FIG. 1 shows an electron beam apparatus embodying the present invention, and the same parts as in FIGS. 2 and 3 are given the same numbers and their explanations will be omitted. The difference between the device shown in FIG. 1 and the conventional device shown in FIG. 2 is that a cylindrical member 8 made of a high-resistance material is placed inside an insulator 5 as a vacuum partition member. be. The cylindrical member is fixed to the anode 3 and the electrode 7 by welding, and the member 8 and both electrodes 3 and 7 are electrically connected. With this configuration, the anode 3 has
Even if the backscattered electrons generated by the collision of the accelerated electron beams head in the direction of the insulator 5, the backscattered electrons collide with the cylindrical member 8 and are immediately discharged through the cylindrical member, which is a high-resistance material. Therefore, the insulator is no longer charged, and creeping discharge on the surface of the insulator can be completely prevented. Further, the role of the vacuum partition wall is played by the insulator 5, and the cylindrical member 8
There is no need to consider vacuum leakage when fixing the cylindrical member 8 to the electrode.
It is sufficient if both ends of the tube are in contact with the electrode metal, and the electrode metal does not diffuse into the cylindrical member at all.
Therefore, the resistance value of the cylindrical member 8 can be maintained at the value when the member was manufactured. Note that a hole 9 is bored in a part of the cylindrical member 8 to increase the exhaust conductance of the space between the cylindrical member 8 and the insulator 5.
以上本考案を詳述したが、本考案は上述した実
施例に限定されず幾多の変型が可能である。例え
ば、本考案を2枚の電極間に高電圧を印加し、荷
電粒子線を集束するようにした静電レンズ部分に
使用することもできる。又、電子線装置を例に説
明したが、本考案をイオンビーム装置に適用する
ことも可能である。 Although the present invention has been described in detail above, the present invention is not limited to the embodiments described above and can be modified in many ways. For example, the present invention can be used in an electrostatic lens part that focuses a charged particle beam by applying a high voltage between two electrodes. Furthermore, although the explanation has been given using an electron beam device as an example, the present invention can also be applied to an ion beam device.
[効果]
以上詳述した如く、本考案は、荷電粒子線の加
速あるいは集束部分に配置される隔壁における沿
面放電を防止することができ、荷電粒子線装置の
正常な動作を長時間に渡つて維持することができ
る。[Effects] As detailed above, the present invention can prevent creeping discharge in the partition wall disposed in the acceleration or focusing portion of the charged particle beam, and can maintain the normal operation of the charged particle beam device for a long time. can be maintained.
第1図は、本考案の一実施例である電子線装置
を示す図、第2図及び第3図は、従来の電子線装
置の一例を示す図である。
1……陰極、2……ウエーネルト電極、3……
陽極、4……高圧電源、5……絶縁碍子、6……
高抵抗物質、7……電極、8……筒状部材、9…
…孔。
FIG. 1 is a diagram showing an electron beam device that is an embodiment of the present invention, and FIGS. 2 and 3 are diagrams showing an example of a conventional electron beam device. 1... cathode, 2... Wehnelt electrode, 3...
Anode, 4... High voltage power supply, 5... Insulator, 6...
High resistance material, 7... Electrode, 8... Cylindrical member, 9...
...hole.
Claims (1)
を印加する手段と、該第1と第2の電極の間の
荷電粒子線通路の周囲に配置される隔壁部材と
を有し、該電極間で荷電粒子線を加速あるいは
集束させるように構成した荷電粒子線装置にお
いて、該隔壁部材の内側に、該隔壁部材から離
間して、高抵抗物質によつて形成された筒状部
材を配置し、該筒状部材と該両電極とを電気的
に接続させたことを特徴とする荷電粒子線装
置。 (2) 該筒状部材には、孔が穿たれている実用新案
登録請求の範囲第1項記載の荷電粒子線装置。[Claims for Utility Model Registration] (1) First and second electrodes, means for applying a high voltage between the two electrodes, and a charged particle beam path between the first and second electrodes. In a charged particle beam device having a partition wall member disposed around the electrodes and configured to accelerate or focus a charged particle beam between the electrodes, a high-voltage beam is provided inside the partition member and spaced apart from the partition wall member. A charged particle beam device characterized in that a cylindrical member made of a resistive material is arranged, and the cylindrical member and both electrodes are electrically connected. (2) The charged particle beam device according to claim 1, wherein the cylindrical member is provided with a hole.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3154787U JPH0521824Y2 (en) | 1987-03-04 | 1987-03-04 |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3154787U JPH0521824Y2 (en) | 1987-03-04 | 1987-03-04 |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS63139757U JPS63139757U (en) | 1988-09-14 |
JPH0521824Y2 true JPH0521824Y2 (en) | 1993-06-04 |
Family
ID=30837386
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3154787U Expired - Lifetime JPH0521824Y2 (en) | 1987-03-04 | 1987-03-04 |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0521824Y2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2010146833A1 (en) * | 2009-06-16 | 2010-12-23 | 株式会社日立ハイテクノロジーズ | Charged particle radiation device |
-
1987
- 1987-03-04 JP JP3154787U patent/JPH0521824Y2/ja not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS63139757U (en) | 1988-09-14 |
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