JPS6014463B2 - electronic microscope - Google Patents
electronic microscopeInfo
- Publication number
- JPS6014463B2 JPS6014463B2 JP55056011A JP5601180A JPS6014463B2 JP S6014463 B2 JPS6014463 B2 JP S6014463B2 JP 55056011 A JP55056011 A JP 55056011A JP 5601180 A JP5601180 A JP 5601180A JP S6014463 B2 JPS6014463 B2 JP S6014463B2
- Authority
- JP
- Japan
- Prior art keywords
- lens
- image
- electron beam
- magnification
- electromagnetic
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/02—Details
- H01J37/04—Arrangements of electrodes and associated parts for generating or controlling the discharge, e.g. electron-optical arrangement or ion-optical arrangement
- H01J37/10—Lenses
- H01J37/14—Lenses magnetic
- H01J37/141—Electromagnetic lenses
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
Description
【発明の詳細な説明】
本発明は透過結像型電子顕微鏡における電子線像の回転
を像倍率とは無関係に独立に制御し得る装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device that can independently control the rotation of an electron beam image in a transmission imaging electron microscope, regardless of the image magnification.
透過結像型電子顕微鏡はその結像レンズ系として複数の
電磁レンズを用いているが、電磁レンズの鞠外対称磁界
によって電子線に対して回転作用が生じ、像倍率を変化
させる操作に伴って姿光坂上に結像する電子線像の視野
が回転する。第1図と第2図は共に通常の電子顕微鏡に
おける結像レンズ系の構成を示す略図であり、レンズ系
の光軸1に沿って薄膜試料2、対物レンズ3、中間レン
ズ4、投影レンズ5及び鞍光板6が順次配置されている
。第1図には高倍率像を得るための電子線経路が描かれ
ており、試料2を透過した電子線が対物レンズ3により
図中7の位置に像を結像し、該像は中間レンズ4により
8の位置に拡大結像され、更に結像は投影レンズ5によ
り発光版6上に投影結像される状態が示されている。第
2図には中倍率像を得るための電子線経路が描かれてお
り、対物レンズ3の励磁か弱く、試料2を透過した電子
線は中間レンズ4の後方8の位置で初めて電子線像を形
成し、該像が投影レンズ5によって姿光板6上に投影さ
れる。これらの図において、各電子線像は全て同一平面
(紙面)にあるように描かれているが、実線には各数は
光軸1に垂直な平面内で電磁レンズの励磁強度に応じた
角度回転するため蟹光坂上に表示される電子線像はその
像倍率が異なると異なった方向で表示されることになる
。そのため試料の同一領域に関して倍率の異なった多数
の電子線像を写真撮影して比較観察する場合などに視野
の方向がバラバラになって不都合を生じる。本発明はこ
のような問題を解決することを目的とするもので、結像
レンズ系内において形成される電子線像の位置又はその
近傍に電磁レンズを設け、該電磁レンズを象回転制御用
として用いることを特徴とするものである。Transmission imaging electron microscopes use multiple electromagnetic lenses as their imaging lens system, but the symmetrical magnetic field of the electromagnetic lenses causes a rotational effect on the electron beam, and as the image magnification is changed, The field of view of the electron beam image formed on the optical slope rotates. Both FIG. 1 and FIG. 2 are schematic diagrams showing the configuration of an imaging lens system in a normal electron microscope, in which a thin film sample 2, an objective lens 3, an intermediate lens 4, a projection lens 5 and a saddle light plate 6 are sequentially arranged. Figure 1 shows the electron beam path for obtaining a high-magnification image. 4, the image is enlarged to the position 8, and the image is further projected onto the light-emitting plate 6 by the projection lens 5. Figure 2 shows the electron beam path for obtaining an intermediate magnification image.The excitation of the objective lens 3 is weak, and the electron beam that passes through the sample 2 forms an electron beam image for the first time at a position 8 behind the intermediate lens 4. The image is projected onto the image light plate 6 by the projection lens 5. In these figures, each electron beam image is drawn as if it were all on the same plane (paper surface), but each number in the solid line is an angle corresponding to the excitation intensity of the electromagnetic lens in a plane perpendicular to optical axis 1. Because of the rotation, the electron beam image displayed on the crab light slope will be displayed in different directions if the image magnification is different. Therefore, when a large number of electron beam images with different magnifications are photographed for the same area of a sample and comparatively observed, the direction of the field of view becomes inconsistent, which causes inconvenience. The purpose of the present invention is to solve such problems by providing an electromagnetic lens at or near the position of the electron beam image formed within the imaging lens system, and using the electromagnetic lens for controlling the rotation of the elephant. It is characterized by its use.
以下図面に基づいて本発明を詳説する。第3図において
、電磁レンズ9(の主面)と物面10の距離aとしンズ
9と後面11の距離bの間にはしンズ9の焦点距離をF
として次のm式が成り立つ。The present invention will be explained in detail below based on the drawings. In FIG. 3, the focal length of the lens 9 is F between the distance a between the electromagnetic lens 9 (principal surface) and the object surface 10 and the distance b between the lens 9 and the rear surface 11.
The following m formula holds true.
貴十毒=音 ‐…‐‐(1〕
{1}式においてaを減少させてF〉aとなると第4図
に示す如くレンズ9の前方に虚像12を形成しb<0と
なる。Kijutoku=sound -...- (1) In the {1} formula, when a is decreased and F>a, a virtual image 12 is formed in front of the lens 9 as shown in FIG. 4, and b<0.
更にaをレンズ9へ近付けると像面bもレンズに近付き
レンズ主面の極く近くに物面があると(a〒0)像面も
略同じ位置となり、像倍率はb/aご1となる。つまり
この場合、レンズは像位置の変化、拡大、縞少の作用を
伴なわすに像に対する回転作用が現われることになる。
本発明は上述の原理を利用するものでありその−実施例
を第5図に示す。When a further approaches the lens 9, the image plane b also approaches the lens, and if the object surface is very close to the main surface of the lens (a〒0), the image plane will also be at approximately the same position, and the image magnification will be equal to b/a by 1. Become. In other words, in this case, the lens exhibits a rotational effect on the image along with the effect of changing the image position, enlarging the image, and reducing the amount of fringes.
The present invention utilizes the principles described above, and an embodiment thereof is shown in FIG.
第5図中第1図及び第2図中に用いたものと同一の数字
を付したものは同一の構成要素を表わしており、従釆例
と異なるのは中間レンズ4の嫁面位置に像回転制御用の
電磁レンズ13が設けられていることである。前記レン
ズ13の励磁を零とした場合の電子線経路を実線14で
示し、レンズ13のレンズコイルへ正負の励磁電流を順
次増加させた場合の電子線経路を破線15と二点鎖線1
6で示す。このようなしンズ13の励磁調整によれば蟹
光板6に結像する電子線像の倍率を一定に保つたまま光
軸1を中心軸として擬位置を任意方向に回転させること
ができる。第5図の装置の場合、投影レンズ5の磁極片
の孔径、間隔が比較的小さい事等に原因して、投影レン
ズ5の極〈近くに他のレンズ13を設けることが実態に
は困難なことも多い。第6図は第5図の装置の欠点を解
決するための実施例を示すもので、投影レンズ5から比
較的離れた位置に像回転制御用の電磁レンズ17と補助
レンズ18を設けたものである。In FIG. 5, the same numbers as those used in FIGS. 1 and 2 represent the same components, and the difference from the conventional example is that the image is placed at the position of the bride surface of the intermediate lens 4. An electromagnetic lens 13 for rotation control is provided. The electron beam path when the excitation of the lens 13 is zero is shown by a solid line 14, and the electron beam path when the positive and negative excitation currents are sequentially increased to the lens coil of the lens 13 is shown by a broken line 15 and a two-dot chain line 1.
6. By adjusting the excitation of the lens 13 in this manner, the pseudo position can be rotated in any direction about the optical axis 1 while keeping the magnification of the electron beam image formed on the crab light plate 6 constant. In the case of the apparatus shown in FIG. 5, it is actually difficult to provide another lens 13 near the pole of the projection lens 5 due to the relatively small hole diameter and spacing of the magnetic pole pieces of the projection lens 5. Often. FIG. 6 shows an embodiment for solving the drawbacks of the device shown in FIG. 5, in which an electromagnetic lens 17 for image rotation control and an auxiliary lens 18 are provided at a position relatively distant from the projection lens 5. be.
図において、中間レンズ4による拡大像は回転制御用レ
ンズ17の主面近傍に結像されるが、該像は補助レンズ
l6によって投影レンズ5の近傍位置19に結像する。
これらの像の倍率は各結像レンズ3,4,5に電流を供
給する結像レンズ電源21を制御する倍率可変手段22
によって可変され鞍光板上に任意の倍率の像を表示する
ことができる。更に第6図の実施例装置においては回転
制御用レンズ17と補助レンズ18のレンズ電源23が
倍率可変手段22からの出力によって制御され、倍率の
可変に伴う釜光板上における電子線像の回転を打ち消す
ように構成されているので、前述した本発明の目的が自
動的に達成される。尚同一倍率において電子線像を回転
させる場合の電子線経路を図中に20,21,22で示
した。In the figure, an enlarged image by the intermediate lens 4 is formed near the main surface of the rotation control lens 17, and the image is formed at a position 19 near the projection lens 5 by the auxiliary lens 16.
The magnification of these images is determined by a magnification variable means 22 that controls an imaging lens power supply 21 that supplies current to each imaging lens 3, 4, and 5.
It is possible to display an image at any magnification on the saddle light plate. Furthermore, in the embodiment shown in FIG. 6, the lens power source 23 for the rotation control lens 17 and the auxiliary lens 18 is controlled by the output from the magnification variable means 22, and the rotation of the electron beam image on the light plate as the magnification is varied is controlled. The objects of the invention described above are automatically achieved. Note that the electron beam paths when rotating the electron beam image at the same magnification are indicated by 20, 21, and 22 in the figure.
第1図及び第2図は電子顕微鏡における結像レンズ系の
作用を説明するための略図、第3図及び第4図は本発明
の原理を説明するための略図、第5図及び第6図は夫々
本発明の実施例装置を示す略図である。
1:光軸、2:試料、3:対物レンズ、4:中間レンズ
、5:投影レンズ、6:姿光板、13,17:回転制御
用レンズ、18:補助レンズ、21:結像レンズ電源、
22:倍率可変手段、23:レンズ電源。
オー図
オZ図
ズろ園
※4図
火5釘
ズ6図Figures 1 and 2 are schematic diagrams for explaining the action of the imaging lens system in an electron microscope, Figures 3 and 4 are schematic diagrams for explaining the principle of the present invention, and Figures 5 and 6 are schematic diagrams for explaining the principle of the present invention. 2A and 2B are schematic diagrams showing embodiment devices of the present invention, respectively. 1: optical axis, 2: sample, 3: objective lens, 4: intermediate lens, 5: projection lens, 6: optical plate, 13, 17: rotation control lens, 18: auxiliary lens, 21: imaging lens power supply,
22: Magnification variable means, 23: Lens power supply. O diagram O Z diagram Zuroen *4 diagram Fire 5 Nails 6 diagram
Claims (1)
ズ以上の電磁レンズから成る結像レンズ系内に、前記中
間レンズによる結像位置またはその近傍をレンズ主面と
する電磁レンズを設け、該電磁レンズの励磁強度を調整
することにより、前記結像レンズ系による電子線像の回
転を制御するように構成したことを特徴とする電子顕微
鏡。1. In an imaging lens system consisting of at least an objective lens, an intermediate lens, and an electromagnetic lens larger than a projection lens, an electromagnetic lens whose main surface is at or near the image formation position by the intermediate lens is provided, and the excitation intensity of the electromagnetic lens is An electron microscope characterized in that it is configured to control rotation of an electron beam image by the imaging lens system by adjusting.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55056011A JPS6014463B2 (en) | 1980-04-26 | 1980-04-26 | electronic microscope |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55056011A JPS6014463B2 (en) | 1980-04-26 | 1980-04-26 | electronic microscope |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56152145A JPS56152145A (en) | 1981-11-25 |
| JPS6014463B2 true JPS6014463B2 (en) | 1985-04-13 |
Family
ID=13015108
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55056011A Expired JPS6014463B2 (en) | 1980-04-26 | 1980-04-26 | electronic microscope |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6014463B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0732108B2 (en) * | 1982-07-28 | 1995-04-10 | 株式会社日立製作所 | Electron beam exposure system |
| JP3782692B2 (en) * | 2001-09-06 | 2006-06-07 | 株式会社東芝 | Electron beam apparatus and semiconductor device manufacturing method using the apparatus |
-
1980
- 1980-04-26 JP JP55056011A patent/JPS6014463B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56152145A (en) | 1981-11-25 |
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