JPS62108439A - Field emission electron gun - Google Patents

Field emission electron gun

Info

Publication number
JPS62108439A
JPS62108439A JP24762885A JP24762885A JPS62108439A JP S62108439 A JPS62108439 A JP S62108439A JP 24762885 A JP24762885 A JP 24762885A JP 24762885 A JP24762885 A JP 24762885A JP S62108439 A JPS62108439 A JP S62108439A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic field
electron beam
chip
electromagnets
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
Application number
JP24762885A
Other languages
Japanese (ja)
Other versions
JPH0656744B2 (en
Inventor
Moriki Kubozoe
窪添 守起
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP60247628A priority Critical patent/JPH0656744B2/en
Publication of JPS62108439A publication Critical patent/JPS62108439A/en
Publication of JPH0656744B2 publication Critical patent/JPH0656744B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Electron Sources, Ion Sources (AREA)

Abstract

PURPOSE:To make it possible to perform the adjustment of an axis by operation from outside as an electron gun housing remains mounted, by providing magnetic poles near an FE chip to apply a two-dimensional magnetic field, and adjusting the magnetic field by operation from outside. CONSTITUTION:Magnetic poles 19, 19' welded to a spacer 20 to withstand a vacuum, electromagnets 18, 18' attached to a circular yoke 17 and the yoke constitute a magnetic circuit. The polarity of the magnets 18, 18' is such that an electron beam emitted from an FE chip 4 is deflected rightward or leftward as to the drawing by a magnetic field generated by the magnetic poles 19, 19'. A similar magnetic circuit extending perpendicularly to the drawing is provided by using the yoke 17 in common to the former magnetic circuit. The magnetic intensity of the electromagnets 18, 18' and other electromagnets, which act perpendicularly to the former, is increased or decreased to two-dimensionally deflect the electron beam in an optional direction. Although a magnetic field is generated because of the presence of the wall of an electron gun housing between the electromagnets 18, 18' and the magnetic poles 19, 19', the magnetic field does not hinder the adjustment of the axis of the electron beam because the magnetic field is distant from the beam.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は電界放射形電子銃に係り、特に透過形電子顕微
鏡に最適な電界放射形電子銃に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a field emission type electron gun, and particularly to a field emission type electron gun most suitable for a transmission electron microscope.

〔発明の背景〕[Background of the invention]

従来、透過型電子類Wi鏡の電界放射形電子銃の構成は
、電子線を放出するFEチップ、電子線を引出すための
電圧Vlを印加する部分と、電子線を加速する電圧Vo
を印加する加速管部とより成つており、これら全体をガ
ンハウジングに収納させている。
Conventionally, the configuration of a field emission type electron gun of a transmission type Wi mirror includes an FE chip that emits an electron beam, a part that applies a voltage Vl to extract the electron beam, and a voltage Vo that accelerates the electron beam.
It consists of an accelerating tube section that applies the electric current, and the entire body is housed in the gun housing.

しかし、FEチップとその他の部分の機械的軸調整が容
易なように配慮されていなかったため。
However, no consideration was given to easy mechanical axis adjustment of the FE chip and other parts.

軸調整のために何度もガンハウジングを開ける繁雑な作
業を行なう必要があった。すなわち、第2図は従来の電
界放射形電子銃の立体断面図、であり。
It was necessary to open the gun housing many times to adjust the shaft, which was a complicated process. That is, FIG. 2 is a three-dimensional cross-sectional view of a conventional field emission type electron gun.

第3図はその主要部の縦断面図である。1はエポキシ樹
脂等の絶縁物で製作されたガンハウジングである。この
中にFEチップ4と引出し電極6よりなる電子線放出部
と電子線を加速する部分、即ちffi極6を含め、電極
7.7’ 、7’と絶縁体5゜5’ 、5’よりなる部
分がある。第2図に示すように高圧ケーブル2には加速
電圧VoをFEチップ4と電極7′の間に印加するため
の芯線と、引出し電圧Vr をFEチップ4と電極6の
間に印加するための芯線が含まれている。電極間には加
速電圧Voを分割して印加するためのブリーダー抵抗1
1.11’ 、11′がある。なお、第3図1点1RI
IAはガンハウジングを示す、ガンハウジング1と電界
放射形電子銃との間の空間3は高電圧絶縁を保つため数
気圧の絶縁ガス(たとえばフレオンガス、SFs等で満
たされている。この状態でvlを印加し、FEチップ4
に係る電界強度が電子線を引出すのに充分なものとなれ
ばFEチップ4の先端から電界放射により電子線が放出
され、電極6の孔12を通って加速管部に電子線が流れ
込んでくる。ここで、加速電圧Voを加速管部に印加す
ると電子線は加速され、最終的にはVoのエネルギーを
持った電子線として加速管部を通過し1図示されてはい
ないが、電界放射形電子銃に接続される鏡体部へと進ん
でゆく。
FIG. 3 is a longitudinal sectional view of the main part. 1 is a gun housing made of an insulating material such as epoxy resin. This includes the electron beam emitting part consisting of the FE chip 4 and the extraction electrode 6, the part that accelerates the electron beam, that is, the ffi pole 6, and the electrodes 7, 7', 7' and the insulators 5°5', 5'. There is a part. As shown in FIG. 2, the high voltage cable 2 includes a core wire for applying an accelerating voltage Vo between the FE chip 4 and the electrode 7', and a core wire for applying the extraction voltage Vr between the FE chip 4 and the electrode 6. Contains core wire. A bleeder resistor 1 is provided between the electrodes to divide and apply the acceleration voltage Vo.
There are 1.11' and 11'. In addition, Fig. 3 1 point 1 RI
IA indicates a gun housing. The space 3 between the gun housing 1 and the field emission type electron gun is filled with several atmospheres of insulating gas (for example, Freon gas, SFs, etc.) to maintain high voltage insulation. In this state, vl FE chip 4
When the electric field intensity becomes sufficient to extract the electron beam, the electron beam is emitted from the tip of the FE chip 4 by field emission, and the electron beam flows into the acceleration tube section through the hole 12 of the electrode 6. . Here, when an accelerating voltage Vo is applied to the accelerating tube section, the electron beam is accelerated and finally passes through the accelerating tube section as an electron beam with energy Vo. Proceed to the mirror body that is connected to the gun.

そこで問題とするところのものは、各電極に電圧が印加
されると、それぞれにレンズ作用を持ち。
The problem here is that when a voltage is applied to each electrode, each electrode has a lens effect.

それらの軸がかならずしも一致しているとは限らないた
めに簡単には電子線が、後に接合された鏡体部の方へ進
行してこないことである。実際の軸31JI!では、ガ
ンハウジング1内の絶縁ガスを大気圧まで減圧し、ネジ
17を全て外してガンマハウジング1を取外すようにし
ている。大気中で。
Because their axes do not necessarily coincide, the simple problem is that the electron beam does not proceed toward the mirror body that is later joined. Actual axis 31JI! Now, the insulating gas inside the gun housing 1 is reduced to atmospheric pressure, all the screws 17 are removed, and the gamma housing 1 is removed. in the atmosphere.

Vl を印加し、ネジ8.9(全部図示されていないが
それぞれ4分割で4本ずつある)を、111!整して電
子線が所望の位置に来るようにする。このとき。
Apply Vl and tighten screws 8.9 (not all shown, but there are 4 pieces each divided into 4 pieces), 111! Adjust the electron beam so that it comes to the desired position. At this time.

ベローズ1oにより、電子銃内は真空に保たれたままF
Eチップ4は、電極6の孔12に対し@調整される。次
にVoをOから徐々に増してゆき、電子線が所定の位置
からずれると同様にし−てネジ8.9で調整する。最初
のうちはVoを印加したままでもよいが1段々Voが高
くなると、 m−7−、*のずれる方向を見定めて、そ
れを補正するように。
The bellows 1o keeps the inside of the electron gun in a vacuum.
The E-tip 4 is aligned with the hole 12 of the electrode 6. Next, gradually increase Vo from O, and if the electron beam deviates from the predetermined position, adjust it in the same way using screw 8.9. At first, Vo can be left applied, but as Vo gradually increases, determine the direction in which m-7-, * shifts and correct it.

一度VoをOFFにしてからネジ8.9で調整する。こ
れを大気圧で放電なしに印加可能な電圧(V oで約2
0kV)まで行う。後は、ガンハウジング1を取り付け
、ネジ17を締付け、3に絶縁ガスを数気圧にまで満す
。しかる後VL を印加し、Vo を大気中で印加した
より高い電圧を印加してゆく。印加の過程で、電子線が
所定の位置から外れたら、その方向を見定めておいて、
 Vt IVo をOFFにし、ガンハウジングを取り
外し、ネジ8,9でVo印加の状態で電子線が所定の位
置に来ると思われる調整を行う。Voは透過電顕では数
百kVであるため、最終加速電圧にまでVoを持って行
って、電子線が所定の位置にあるようにするためには、
前述の過程を数10回繰返す必要がある。経験と感によ
りこの回数は減せることができるのであろうが、決して
容易な作業ではない。
Turn Vo off once and adjust with screw 8.9. This is the voltage that can be applied without discharge at atmospheric pressure (approximately 2 V o
0kV). After that, attach the gun housing 1, tighten the screws 17, and fill the chamber 3 with insulating gas to several atmospheres. Thereafter, VL is applied, and Vo is applied at a higher voltage than that applied in the atmosphere. If the electron beam deviates from the specified position during the application process, determine its direction and
Turn off Vt IVo, remove the gun housing, and use screws 8 and 9 to make adjustments that will bring the electron beam to a predetermined position with Vo applied. Since Vo is several hundred kV in a transmission electron microscope, in order to bring Vo to the final accelerating voltage so that the electron beam is at a predetermined position,
It is necessary to repeat the above process several dozen times. It may be possible to reduce this number with experience and intuition, but it is by no means an easy task.

〔発明の目的〕[Purpose of the invention]

本発明の目的は軸調整の容易な電界型放射電子銃を提供
するにある。
An object of the present invention is to provide a field type radiation electron gun whose axis can be easily adjusted.

〔発明の概要〕[Summary of the invention]

透過形電子顕微鏡の加速電圧は100kV以上と高いた
め、fw界梨型放射電子銃全体ガンハウジング内に収納
されているが、このガンハウジングを取り付けたまま、
磁界を利用してその外部から軸W7149!iiができ
る構造とするようにしたものである。
Since the accelerating voltage of a transmission electron microscope is as high as 100 kV or more, the entire fw Kairi-type radiation electron gun is housed inside the gun housing, but with this gun housing attached,
Axis W7149 from the outside using a magnetic field! The structure is such that ii can be achieved.

〔発明の実施例〕[Embodiments of the invention]

第1図は本発明による電界放射形電子銃の一実施例を示
す構成図である。第2図と同符号のものは同機能を有す
る。まず通常電子銃の電子線体は非常に細いため、外部
交流磁界の影響を受は易い。
FIG. 1 is a block diagram showing an embodiment of a field emission type electron gun according to the present invention. Components with the same symbols as in FIG. 2 have the same functions. First, since the electron beam body of an electron gun is usually very thin, it is easily affected by external alternating magnetic fields.

従って、これを防ぐため、flE極6,7.7’ 、7
’等はパーマロイ等の磁性体で製作されているが。
Therefore, in order to prevent this, flE poles 6, 7.7', 7
' etc. are made of magnetic materials such as permalloy.

この実施例では、電極6を非磁性のSUS材を用いる。In this embodiment, the electrode 6 is made of a non-magnetic SUS material.

19.19’は円筒状のパーマロイ棒を図のように成形
し磁極としたものである。19゜19′はスペーサー2
0に耐真空的に溶接、されており、加速管内は真空に保
持される。17は円形ヨークであり、これに電磁石18
.18’ が取り付けられている。18.19.19’
 、1B’ 。
19.19' is a cylindrical permalloy rod formed as a magnetic pole as shown in the figure. 19°19' is spacer 2
The inside of the accelerator tube is maintained in a vacuum. 17 is a circular yoke, to which an electromagnet 18 is attached.
.. 18' is attached. 18.19.19'
, 1B'.

17で磁気回路が形成される。電磁石18.18’の極
性は、磁極19.19’で形成する磁界により、FEチ
ップ4から数量される電子線を紙面上、左右に偏向でき
るようにする。図示されていないが、同様の磁気回路を
ヨーク17を共通にして、紙面に垂直な方向にも設けで
ある。これにより、電磁石18.18’とこれに垂直な
1個の電磁石の強さを加減することにより、電子線を2
次元的に任意の方向に偏向させることができる。18と
19の117.19’ と18′の間にはガンハウジン
グの壁が存在するためその部分は磁気的にはギャップが
できて、磁界が発生するが、電子線からは遠い位置であ
るので、電子線の軸W整に支障をきたすようなことはな
い。
A magnetic circuit is formed at 17. The polarity of the electromagnets 18, 18' is such that the electron beam emitted from the FE chip 4 can be deflected to the left or right on the paper by the magnetic field formed by the magnetic poles 19, 19'. Although not shown, a similar magnetic circuit is also provided in the direction perpendicular to the plane of the paper, using the yoke 17 in common. As a result, by adjusting the strength of the electromagnet 18, 18' and one electromagnet perpendicular to it, the electron beam can be
It can be deflected dimensionally in any direction. 18 and 19 117. Since there is a wall of the gun housing between 19' and 18', there is a magnetic gap in that part and a magnetic field is generated, but it is located far from the electron beam. , there is no problem in aligning the axis W of the electron beam.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明によれば、電子銃の軸調整に
おいて、ガンハウジングを付けたり外したりの手間がな
く、軸調整に要する時間は従来の数10分の1ですみ、
その効率の向上は顕著である。
As explained above, according to the present invention, when adjusting the axis of an electron gun, there is no need to attach or remove the gun housing, and the time required for axis adjustment is several tenths of that of the conventional one.
The improvement in efficiency is remarkable.

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

第1図は本発明による電界放射形電子銃の一実施例を示
す構成図、第2図は従来の電界放射形電子鏡の立体断面
図、第3図は第2図の主要部分の縦断面図に電気回路を
加えた図である。 1・・・ガンハウジング、2・・・高圧ケーブル53・
・・空間、4・・・FEチップ、5.5’ 、5’・・
・絶縁物。 6・・・引出し電極、7.7’ 、7’・・・電極、8
・・・ネジ、9・・・ネジ、10・・・ベローズ、11
.11’ 。 111・・・ブリーダー抵抗、12・・・孔、13・・
・コンタクト、14.15・・・バネ、16・・・コン
タクト、17・・・ネジ、18・・・絶縁体。
FIG. 1 is a configuration diagram showing an embodiment of a field emission type electron gun according to the present invention, FIG. 2 is a three-dimensional sectional view of a conventional field emission type electron mirror, and FIG. 3 is a vertical cross section of the main part of FIG. 2. It is a diagram in which an electric circuit is added to the diagram. 1...Gun housing, 2...High voltage cable 53.
...Space, 4...FE chip, 5.5', 5'...
·Insulator. 6... Extraction electrode, 7.7', 7'... Electrode, 8
...Screw, 9...Screw, 10...Bellows, 11
.. 11'. 111... Bleeder resistance, 12... Hole, 13...
- Contact, 14.15... Spring, 16... Contact, 17... Screw, 18... Insulator.

Claims (1)

【特許請求の範囲】[Claims] 1、ガンハウジングの内部に少なくとも、FEチップ、
引出し電極、複数段の加速管と、引出し電圧、加速電圧
印加可能な構造を備えた電界放射形電子銃において、該
FEチップの近傍に2次元的な磁界を加えるように磁極
を設け、該磁極の磁界を外部から加減することにより、
FEチップから放出される電子線を2次元的に偏向可能
にしたことを特徴とする電界放射形電子銃。
1. At least an FE chip inside the gun housing,
In a field emission type electron gun equipped with an extraction electrode, a plurality of stages of acceleration tubes, and a structure capable of applying an extraction voltage and an acceleration voltage, a magnetic pole is provided to apply a two-dimensional magnetic field near the FE chip, and the magnetic pole is By adjusting the magnetic field from the outside,
A field emission type electron gun characterized in that an electron beam emitted from an FE chip can be deflected two-dimensionally.
JP60247628A 1985-11-05 1985-11-05 Field emission electron gun Expired - Lifetime JPH0656744B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60247628A JPH0656744B2 (en) 1985-11-05 1985-11-05 Field emission electron gun

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60247628A JPH0656744B2 (en) 1985-11-05 1985-11-05 Field emission electron gun

Publications (2)

Publication Number Publication Date
JPS62108439A true JPS62108439A (en) 1987-05-19
JPH0656744B2 JPH0656744B2 (en) 1994-07-27

Family

ID=17166335

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60247628A Expired - Lifetime JPH0656744B2 (en) 1985-11-05 1985-11-05 Field emission electron gun

Country Status (1)

Country Link
JP (1) JPH0656744B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02113257U (en) * 1988-05-24 1990-09-11

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5034461A (en) * 1973-07-31 1975-04-02

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5034461A (en) * 1973-07-31 1975-04-02

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02113257U (en) * 1988-05-24 1990-09-11

Also Published As

Publication number Publication date
JPH0656744B2 (en) 1994-07-27

Similar Documents

Publication Publication Date Title
US2305884A (en) Electron beam concentrating system
JP6198211B2 (en) Plasma source apparatus and method for generating a charged particle beam
JP5822767B2 (en) Ion source apparatus and ion beam generating method
US2212206A (en) Electron device
WO1997037519A1 (en) Plasma accelerator
US3581093A (en) Dc operated positive ion accelerator and neutron generator having an externally available ground potential target
JPH04233144A (en) Improved magnet for drift of x-ray tube
US4339694A (en) Flat cathode ray tube
US6242749B1 (en) Ion-beam source with uniform distribution of ion-current density on the surface of an object being treated
JPS62108439A (en) Field emission electron gun
JPH07161323A (en) Ion source
US3646379A (en) X-ray tube having controllable focal spot size
EP2446456B1 (en) Magnetically insulated cold-cathode electron gun
US2898493A (en) Method and apparatus for controlling electron beams
US3034012A (en) Electron gun assemblies
JP2000090866A (en) Electron gun, electron beam generating method by electron gun, and exposing device using electron gun
US3316432A (en) Cathode ray tube electron gun mount with unitary magnetic centering and gettering means
US4032815A (en) Collimated beam electron gun system for shaped beam cathode ray tube
US3366904A (en) High-power multi-stage klystron with adjustable periodic magnetic focussing
US4445070A (en) Electron gun for producing spiral electron beams and gyrotron devices including same
US3914637A (en) Method and apparatus for focusing an electron beam
GB679348A (en) Improvements in or relating to cathode ray tubes
US2931903A (en) Acceleration and application of high intensity electron beams for radiation processing
US2876376A (en) Magnetron beam switching tube
US3192425A (en) X-ray tube with adjustable electron beam cross-section