JPH0479139A - Exb-type energy filter - Google Patents

Exb-type energy filter

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Publication number
JPH0479139A
JPH0479139A JP2191928A JP19192890A JPH0479139A JP H0479139 A JPH0479139 A JP H0479139A JP 2191928 A JP2191928 A JP 2191928A JP 19192890 A JP19192890 A JP 19192890A JP H0479139 A JPH0479139 A JP H0479139A
Authority
JP
Japan
Prior art keywords
electric field
magnetic poles
voltage
magnetic pole
electrodes
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
JP2191928A
Other languages
Japanese (ja)
Inventor
Katsushige Tsuno
勝重 津野
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.)
Jeol Ltd
Original Assignee
Jeol 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 Jeol Ltd filed Critical Jeol Ltd
Priority to JP2191928A priority Critical patent/JPH0479139A/en
Publication of JPH0479139A publication Critical patent/JPH0479139A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To prevent the disorder of electric field distribution owing to the presence of magnetic poles made of a metal magnetic material by putting magnetic poles divided by planes rectangular to an electric field in the electric field rectangularly and applying electric voltage controllably to the magnetic poles with the same polarity as the voltage applied to the electrodes of the electric field nearest each of the divided magnetic poles and lower than that applied to the electric field electrodes. CONSTITUTION:Magnetic poles 1a, 1b and magnetic poles 2a, 2b divided by planes rectangular to an (x) direction of an electric field are put in the opposite each other rectangularly to the electric field. Voltage +Va, -Va with the same polarity of voltage +V or -V applied to the electrodes 3 or 3' of an electric field nearest each of the magnetic poles and at highest one second of voltage applied to the electrodes of the electric field is applied to each of the divided magnetic poles from electric power sources 8a, 8b for magnetic poles. Consequently, the electric field distribution formed by the voltage +V and -V applied to the electrodes 3, 3' of the electric field can be corrected by voltage value +Va, -Va applied to the magnetic poles la, 2a and the magnetic poles 1b, 2b and parallel degree to the x-axis is improved and uniform electric field distribution is obtained.

Description

【発明の詳細な説明】 [産業上の利用分野コ 本発明は、電場と磁場が互いに直交して形成されている
重畳場を有するE×B型エネルギーフィルタに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an E×B type energy filter having a superimposed field in which an electric field and a magnetic field are formed orthogonally to each other.

[従来の技術] 従来、電場と磁場を直交させ、この重畳場に直交する方
向に荷電粒子を直進させることによってエネルギー分析
を行なうE×B型エネルギーフィルタ(以下、単にエネ
ルギーフィルタと称す)が知られている。このようなエ
ネルギーフィルタの構造については種々提案されている
が、電子顕微鏡等の光軸中に接続または挿入して使用さ
れるエネルギーフィルタを第3図(a)〜(c)に基づ
いて説明する。第3図において10.10−は磁極片、
11.11−は電場電極である。
[Prior Art] Conventionally, an E×B type energy filter (hereinafter simply referred to as an energy filter) is known, which performs energy analysis by orthogonalizing an electric field and a magnetic field and causing charged particles to travel straight in a direction perpendicular to this superimposed field. It is being Although various structures of such energy filters have been proposed, an energy filter used by being connected or inserted into the optical axis of an electron microscope, etc. will be explained based on FIGS. 3(a) to (c). . In Fig. 3, 10.10- is a magnetic pole piece,
11.11- is an electric field electrode.

第3図(a)に示すエネルギーフィルタは荷電粒子線の
光軸2に対して互いに直交する電場と磁場を与え、電場
による荷電粒子の偏向を磁場による偏向で打ち消し、入
射した荷電粒子線の内ある特定のエネルギーを持った粒
子が選択的に直進されるように構成されている。
The energy filter shown in Fig. 3(a) applies an electric field and a magnetic field perpendicular to each other to the optical axis 2 of the charged particle beam, cancels the deflection of the charged particles due to the electric field with the deflection due to the magnetic field, and absorbs the incident charged particle beam. It is configured so that particles with a certain energy are selectively moved straight.

第3図(a)に示すような構成によれば、エネルギーフ
ィルタの内部では勿論のこと、フリンジ場、即ちエネル
ギーフィルタにおける電子線の入射部および出射部にお
いてもウィーン条件を満足できる。つまり、エネルギー
フィルタにおいては荷電粒子を直進させる必要があり、
電場をE、磁場を85荷電粒子の速度をVとしたとき、
Emv・Bというウィーン条件を満足しなければならな
い。但し、E、BSVはいずれもベクトルである。
According to the configuration shown in FIG. 3(a), the Wien condition can be satisfied not only inside the energy filter but also in the fringe field, that is, the entrance and exit parts of the electron beam in the energy filter. In other words, in an energy filter, charged particles must travel straight,
When the electric field is E, the magnetic field is 85, and the velocity of the charged particle is V,
The Vienna condition of Emv.B must be satisfied. However, both E and BSV are vectors.

しかし、前記電場および磁場に−様な電場と磁場を用い
たエネルギーフィルタに、第4図(a)に示すように荷
電粒子線、例えば電子線が入射された場合、該電子線は
電場方向には収束されるが、磁場方向には収束作用を持
たずに発散するため、エネルギーフィルタに断面が円形
の電子線を入射した場合でも、円弧状の電子線、即ち非
点を有する電子線が出射されてしまう。この欠点を補う
ために、第3図(b)に示すような傾斜磁場型のフィル
タや同図(c)に示すような弧状電極型フィルタなどが
提案されている。これらのフィルタでは、電場Ex、磁
場By、を次のような式E x = E o  (1+
 a 、x 十a 2 x 2+−)  式■By−B
o  (1+b、y+b2y2+−)  式■で表した
とき、b1項または81項が夫々付加され、この成分に
よってX方向への収束作用が遅らされると共に、X方向
への収束作用が発生し、適切な31項またはb1項また
は両頂の組み合わせにより、第4図(b)に示すような
x、X方向の軌道を一致させた非点のない像が得られる
ことが知られている。なお、この非点なし結像を与える
81項またはb1項の値は、フィルタ長りによって決定
される。
However, when a charged particle beam, for example an electron beam, is incident on an energy filter using an electric field and a magnetic field similar to the electric field and magnetic field as shown in FIG. is converged, but diverges without having a convergence effect in the direction of the magnetic field, so even if an electron beam with a circular cross section is incident on an energy filter, an arc-shaped electron beam, that is, an electron beam with astigmatism will be emitted. It will be done. In order to compensate for this drawback, a gradient magnetic field type filter as shown in FIG. 3(b) and an arc electrode type filter as shown in FIG. 3(c) have been proposed. In these filters, the electric field Ex and the magnetic field By are expressed as follows: Ex = E o (1+
a , x 10a 2 x 2+-) Formula ■By-B
o (1+b, y+b2y2+-) When expressed by formula (■), the b1 term or the 81st term is added, and this component delays the convergence effect in the X direction, and also causes the convergence effect in the X direction, It is known that by using an appropriate 31 term or b1 term or a combination of both vertices, it is possible to obtain an image without astigmatism with matching trajectories in the x and X directions as shown in FIG. 4(b). Note that the value of the 81 term or the b1 term that provides this astigmatic imaging is determined by the filter length.

[発明か解決しようとする課題] 上述したようなエネルギーフィルタにおいては、通常は
前記82項およびb1項のみが考慮されて設計がなされ
ているが、鉄等の金属磁性材料から成る磁極片と銅等の
非磁性金属材料で形成された電極から成るエネルギーフ
ィルタについて前記各係数の一例を求めると、83項お
よびb1項か、a、 =0.005 mm−’、  b
z −0,275mm−’であるのに対して82項およ
びb2項はa2−0.039 mm−’、  b2−−
0.0022 mm−’となっている。ここで、82項
およびb2項の値(絶対値)に着目すると、82項の値
の方がb2項よりも1桁以上大きな値を取ることかわか
る。このように、82項が大きな値を持つ場合、フィル
ター内の電界分布は第5図に破線で示すように磁極の中
心付近と、周辺部分とで大きさが異なり、電子線が光軸
から少しでも外れた位置に入射した場合には、フィルタ
ー内での電子軌道は乱され、所望のエネルギーの電子を
光軸に沿って選択的に通過させることができなくなる。
[Problem to be solved by the invention] In the energy filter as described above, normally only the above-mentioned terms 82 and b1 are taken into consideration when designing, but the magnetic pole piece made of a metal magnetic material such as iron and copper When determining an example of each of the above coefficients for an energy filter consisting of electrodes made of non-magnetic metal materials such as 83 terms and b1 terms, a, =0.005 mm-', b
z -0,275 mm-', whereas the 82nd term and b2 term are a2-0.039 mm-', b2--
It is 0.0022 mm-'. Here, if we pay attention to the values (absolute values) of the 82nd term and the b2 term, we can see that the value of the 82nd term is one or more orders of magnitude larger than the b2 term. In this way, when the 82 term has a large value, the electric field distribution inside the filter differs in magnitude between the center of the magnetic pole and the periphery, as shown by the broken line in Figure 5, and the electron beam is slightly deviated from the optical axis. However, if the electrons are incident at a different position, the electron trajectory within the filter will be disturbed, making it impossible to selectively pass electrons with the desired energy along the optical axis.

この電界分布の不均一性の理由としては、まず第1に磁
極片を傾斜させたことにより、片側の電極の表面積が小
さくなったことがあげられる。そして、第2には磁場の
形成は対向する磁極片のみに寄与しているものの、電場
の形成は電圧の印加される電極以外に、接地電位にある
前記磁極片が電場に略平行に配置されていることにより
、−様な場か乱されると考えられる。
The reason for the non-uniformity of the electric field distribution is that, first, by tilting the magnetic pole pieces, the surface area of one electrode becomes smaller. Second, although the formation of a magnetic field contributes only to the opposing magnetic pole pieces, the formation of an electric field is caused by the fact that, in addition to the electrodes to which voltage is applied, the magnetic pole pieces at ground potential are placed approximately parallel to the electric field. It is thought that the situation is disrupted in a negative way.

本発明は、上述した問題点を考慮し、金属磁性材料製の
磁極片の存在による電場分布の乱れを少なくすることの
できる、E×B型エネルギーフィルタを提供することを
目的としている。
The present invention has been made in consideration of the above-mentioned problems, and an object of the present invention is to provide an E×B type energy filter that can reduce disturbances in electric field distribution due to the presence of magnetic pole pieces made of metal magnetic material.

[課題を解決するための手段] 本発明は、電場と磁場が互いに直交して形成されてなる
E×B型エネルギーフィルタにおいて、電場に直交する
面によって分割された磁極片を前記電場に直交して配置
すると共に、前記分割された各磁極片に各磁極片に最も
近い側の電場電極に印加される電圧と同極性で、且つ電
場電極に印加される電圧よりも低い電圧を調整可能に印
加したことを特徴としている。
[Means for Solving the Problems] The present invention provides an E×B type energy filter in which an electric field and a magnetic field are formed orthogonal to each other, in which magnetic pole pieces divided by a plane orthogonal to the electric field are arranged orthogonal to the electric field. At the same time, a voltage having the same polarity as the voltage applied to the electric field electrode closest to each magnetic pole piece and lower than the voltage applied to the electric field electrode is applied to each of the divided magnetic pole pieces in an adjustable manner. It is characterized by what it did.

[実施例コ 以下、本発明の実施例を図面に基づいて説明する。第1
図は本発明の一実施例によるE×B型エネルギーフィル
タの構成図、第2図は各電極および磁極片への電圧の印
加方法を説明するための図である。
[Embodiments] Hereinafter, embodiments of the present invention will be described based on the drawings. 1st
The figure is a block diagram of an E×B type energy filter according to an embodiment of the present invention, and FIG. 2 is a diagram for explaining a method of applying voltage to each electrode and a magnetic pole piece.

第1図および第2図において、1alb、2a、2bは
磁極片、3.3′は電極、4a、4bはヨーク、5,6
は励磁コイル、7は電場電源、8a、8bは磁極片間用
電源である。
1 and 2, 1alb, 2a, 2b are magnetic pole pieces, 3.3' are electrodes, 4a, 4b are yokes, 5, 6
7 is an excitation coil, 7 is an electric field power supply, and 8a and 8b are power supplies for between magnetic pole pieces.

電場方向Xに直交する面によって分割された磁極片1a
、lbと磁極片2a、2bは前記電場に直交して対向し
て配置されている。磁極片1aおよび2aはヨーク4a
の両端部に接続され、磁極片1bおよび2bはヨーク4
bの両端部に接続されており、磁極片1aおよび1bは
励磁コイル5によってS極を生じるように励磁され、磁
極片2aおよび2bは励磁コイル6によってN極を生じ
るように励磁されている。ここで、励磁コイル5゜6は
ヨーク4a及び4bに対しては電気的に絶縁されている
。そして、前記分割された磁極片の夫々には各磁極片に
最も近い側の電場電極3または3゛に印加される電圧+
Vまたは=■と同極性で、且つ該電場電極に印加される
電圧の2分の1以下の電圧+Va、−Vaが磁極片間用
電源8a、8bから印加されている。
A magnetic pole piece 1a divided by a plane perpendicular to the electric field direction
, lb and the magnetic pole pieces 2a, 2b are arranged facing each other orthogonally to the electric field. The magnetic pole pieces 1a and 2a are the yoke 4a
The magnetic pole pieces 1b and 2b are connected to both ends of the yoke 4.
The magnetic pole pieces 1a and 1b are excited by the excitation coil 5 to generate an S pole, and the magnetic pole pieces 2a and 2b are excited by the excitation coil 6 to generate an N pole. Here, the excitation coil 5°6 is electrically insulated from the yokes 4a and 4b. Each of the divided magnetic pole pieces is applied with a voltage +
Voltages +Va and -Va, which have the same polarity as V or =■ and are less than half of the voltage applied to the electric field electrodes, are applied from the power supplies 8a and 8b for between the pole pieces.

なお、傾斜された磁極片1a、lbおよび2a2bの傾
斜角度は、■式のす3項の値にのみ関係するものであり
、82項およびb2項の導出とは独立して扱うことかで
きるため、第2図においては磁極片の傾斜を無視し、簡
略化した電極と磁極片の構成図面に基づいて、各電極お
よび磁極片への電圧の印加方法を説明している。
Note that the angle of inclination of the tilted magnetic pole pieces 1a, lb, and 2a2b is related only to the value of the third term in equation (2), and can be treated independently from the derivation of the 82nd term and the b2 term. In FIG. 2, the method of applying voltage to each electrode and pole piece is explained based on a simplified diagram of the structure of the electrode and pole piece, ignoring the inclination of the pole piece.

第2図に示すような構成のエネルギーフィルタの場合1
.電場電極は6極構成となる。そのため、電場電極3.
3′に印加される電圧+VおよびVによって形成される
電場の分布は、磁極片1a。
In the case of an energy filter with the configuration shown in Figure 2 1
.. The electric field electrode has a six-pole configuration. Therefore, electric field electrode 3.
The distribution of the electric field formed by the voltage +V and V applied to the pole piece 1a.

2aおよび磁極片1b、2bに印加される電圧値+Va
、 −Vaによって補正され、第5図に実線で示すよう
に、X軸に対する平行度か改善される。
2a and the voltage value +Va applied to the magnetic pole pieces 1b, 2b
, -Va, and the parallelism with respect to the X axis is improved as shown by the solid line in FIG.

このように、金属磁性材料によって形成される磁極片が
存在する場合でも、電場分布の乱れを外部より補正する
ことができるため、前述した0式82項の値を極めて小
さくすることができる。
In this way, even if there is a magnetic pole piece made of a metallic magnetic material, disturbances in the electric field distribution can be corrected from the outside, so the value of the above-mentioned equation 82 can be made extremely small.

なお、上述した実施例は本発明の一実施例に過ぎず、本
発明は種々変形して実施することかできる。例えば上述
した実施例においては、励磁コイル5および6を夫々ヨ
ーク4a、4b間に掛は渡して、分割された磁極片を励
磁するようにしたか、ヨーク4aに接続された磁極片1
a、2aおよびヨーク4bに接続された磁極片1b、2
bを個々に励磁するコイルをヨーク4a側および4b側
に設けても良い。
Note that the embodiment described above is only one embodiment of the present invention, and the present invention can be implemented with various modifications. For example, in the embodiment described above, the excitation coils 5 and 6 are passed between the yokes 4a and 4b to excite the divided magnetic pole pieces, or the magnetic pole piece 1 connected to the yoke 4a is
a, 2a and magnetic pole pieces 1b, 2 connected to the yoke 4b.
Coils that individually excite b may be provided on the yoke 4a side and the yoke 4b side.

また、上述した実施例において、電場電極33′は対向
する一対の電極として構成されたが、該電極は分割され
た二対の電極として構成されていても良い。この場合、
各電極に印加される電圧は独立に調整される。
Further, in the above-described embodiment, the electric field electrodes 33' are configured as a pair of electrodes facing each other, but the electrodes may be configured as two pairs of divided electrodes. in this case,
The voltage applied to each electrode is adjusted independently.

[発明の効果コ 以上の説明から明らかなように、本発明は、電場と磁場
が互いに直交して形成されてなるE×B型エネルギーフ
ィルタにおいて、電場に直交する面によって分割された
磁極片を前記電場に直交して配置すると共に、前記分割
された各磁極片に各磁極片に最も近い側の電場電極に印
加される電圧と同極性で、且つ電場電極に印加される電
圧よりも低い電圧を調整可能に印加したことにより、8
2項の値を外部より変化させることができるようになり
、均一な電場分布を得ることができる。
[Effects of the Invention] As is clear from the above description, the present invention provides an E×B type energy filter in which an electric field and a magnetic field are formed orthogonally to each other, in which magnetic pole pieces are divided by a plane orthogonal to the electric field. A voltage that is arranged perpendicular to the electric field and has the same polarity as the voltage applied to the electric field electrode closest to each of the divided magnetic pole pieces, and is lower than the voltage applied to the electric field electrode. By adjusting the application of 8
The value of the second term can now be changed externally, and a uniform electric field distribution can be obtained.

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

第1図は本発明の一実施例によるE×B型エネルギーフ
ィルタの構成図、第2図は各電極および磁極片への電圧
の印加力法を説明するための図、第3図(a)乃至(c
)は従来のE×B型エネルギーフィルタを説明するため
の図、第4図(a)(b)はエネルギーフィルタ内での
電子の軌道を示す図、第5図はエネルギーフィルタ内の
電場分布を説明するための図である。 la、lb、2a、2b:磁極片 3.3−:電極 4a  4b:ヨーク 5.6:励磁コイル 7;電場電源 8a、8b:磁極片間用電源
Fig. 1 is a configuration diagram of an E×B type energy filter according to an embodiment of the present invention, Fig. 2 is a diagram for explaining the method of applying voltage to each electrode and magnetic pole piece, and Fig. 3 (a) ~(c
) is a diagram for explaining the conventional E×B type energy filter, Figures 4(a) and (b) are diagrams showing the trajectory of electrons within the energy filter, and Figure 5 is a diagram showing the electric field distribution within the energy filter. It is a figure for explaining. la, lb, 2a, 2b: magnetic pole piece 3.3-: electrode 4a 4b: yoke 5.6: excitation coil 7; electric field power source 8a, 8b: power source between magnetic pole pieces

Claims (1)

【特許請求の範囲】[Claims]  電場と磁場が互いに直交して形成されてなるE×B型
エネルギーフィルタにおいて、電場に直交する面によっ
て分割された磁極片を前記電場に直交して配置すると共
に、前記分割された各磁極片に各磁極片に最も近い側の
電場電極に印加される電圧と同極性で、且つ電場電極に
印加される電圧よりも低い電圧を調整可能に印加したこ
とを特徴とするE×B型エネルギーフィルタ。
In an E×B type energy filter in which an electric field and a magnetic field are formed orthogonally to each other, magnetic pole pieces divided by a plane perpendicular to the electric field are arranged perpendicular to the electric field, and each divided magnetic pole piece has An E×B type energy filter characterized in that a voltage having the same polarity as the voltage applied to the electric field electrode closest to each magnetic pole piece and lower than the voltage applied to the electric field electrode is applied in an adjustable manner.
JP2191928A 1990-07-20 1990-07-20 Exb-type energy filter Pending JPH0479139A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2191928A JPH0479139A (en) 1990-07-20 1990-07-20 Exb-type energy filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2191928A JPH0479139A (en) 1990-07-20 1990-07-20 Exb-type energy filter

Publications (1)

Publication Number Publication Date
JPH0479139A true JPH0479139A (en) 1992-03-12

Family

ID=16282778

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2191928A Pending JPH0479139A (en) 1990-07-20 1990-07-20 Exb-type energy filter

Country Status (1)

Country Link
JP (1) JPH0479139A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002190273A (en) * 2000-12-22 2002-07-05 Anelva Corp Electromagnetic field superimposed sector type spectroscope
JP2008293977A (en) * 2007-05-24 2008-12-04 Ceos Corrected Electron Optical Systems Gmbh Monochromator and radiation source equipped with monochromator

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002190273A (en) * 2000-12-22 2002-07-05 Anelva Corp Electromagnetic field superimposed sector type spectroscope
JP2008293977A (en) * 2007-05-24 2008-12-04 Ceos Corrected Electron Optical Systems Gmbh Monochromator and radiation source equipped with monochromator

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