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JPH039581B2 - - Google Patents
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JPH039581B2 - - Google Patents

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Publication number
JPH039581B2
JPH039581B2 JP59112469A JP11246984A JPH039581B2 JP H039581 B2 JPH039581 B2 JP H039581B2 JP 59112469 A JP59112469 A JP 59112469A JP 11246984 A JP11246984 A JP 11246984A JP H039581 B2 JPH039581 B2 JP H039581B2
Authority
JP
Japan
Prior art keywords
lens
charged particle
image
hole
electron
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
Application number
JP59112469A
Other languages
Japanese (ja)
Other versions
JPS60257053A (en
Inventor
Toyoki Kitayama
Shigeru Morya
Kazuhiko Komatsu
Toshinori Goto
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.)
NTT Inc
Original Assignee
Nippon Telegraph and Telephone Corp
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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP59112469A priority Critical patent/JPS60257053A/en
Publication of JPS60257053A publication Critical patent/JPS60257053A/en
Publication of JPH039581B2 publication Critical patent/JPH039581B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/30Electron-beam or ion-beam tubes for localised treatment of objects
    • H01J37/3002Details
    • H01J37/3007Electron or ion-optical systems

Landscapes

  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Electron Beam Exposure (AREA)

Description

【発明の詳細な説明】 本発明は荷電粒子レンズの像面に多極子荷電粒
子レンズを配置させた荷電粒子ビーム装置に関す
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a charged particle beam device in which a multipole charged particle lens is arranged on the image plane of the charged particle lens.

最近、電子ビームやイオンビームを使つて材料
上にパターンを描画するいわゆる荷電粒子ビーム
描画装置が(超)LSI素子等の製作手段として脚
光を浴びている。電子ビーム描画装置を例に取つ
て説明すると、該装置にはスポツト状のビームを
材料上の所定の位置に結像させてパターンを描画
する方式のもの(スポツト型電子ビーム描画装
置)、ビーム通路上に正方形又は矩形状の孔を有
するマスク板を置くことにより断面形状が正方形
又は矩形状に整形されたビームを材料上の所定の
位置に結像させてパターンを描画する方式もの
(固定面積型電子ビーム描画装置)、ビーム通路上
に複数枚の前記の如きマスク板を置き、各マスク
板間に置かれた偏向器をコントロールすることに
より最終マスク板を通過するビームの断面形状及
び大きさを可変出来る様になし、該最終マスク板
を通過したビームを材料上の所定の位置に結像さ
せてパターンを描画する方式のもの(可変面積型
電子ビーム描画装置)等がある。
Recently, so-called charged particle beam lithography systems, which draw patterns on materials using electron beams or ion beams, have been in the spotlight as a means of manufacturing (super)LSI devices. Taking an electron beam lithography system as an example, this system includes one that draws a pattern by focusing a spot-shaped beam on a predetermined position on a material (spot-type electron beam lithography system), and a beam path. A method in which a pattern is drawn by placing a mask plate with square or rectangular holes on top of the material and focusing a beam whose cross section is square or rectangular at a predetermined position on the material (fixed area type). (electron beam lithography system), a plurality of mask plates as described above are placed on the beam path, and the cross-sectional shape and size of the beam passing through the final mask plate are controlled by controlling the deflector placed between each mask plate. There is a system (variable area type electron beam lithography system) in which a pattern is drawn by imaging a beam that has passed through the final mask plate at a predetermined position on the material.

本発明は、前述のような装置において、ターゲ
ツト上に照射される荷電ビームの断面形状をマス
クの孔の形状に制約されずに任意に可変とする荷
電粒子ビームを提供することを目的としており、
そのため本発明は、荷電粒子ビーム発生手段、該
発生手段からの荷電粒子ビーム通路上に配置され
ビーム断面整形用の孔を有するマスク板、荷電粒
子ビームによる孔の像を結像させるための第1の
荷電粒子レンズ、該第1の荷電粒子レンズによつ
て結像された荷電粒子ビームによる前記孔の像を
ターゲツト上に結像する為の第2の荷電粒子レン
ズを備えた荷電粒子ビーム装置において、前記第
1のレンズによる孔の像の結像面に配置された多
極子荷電粒子レンズ、該多極子荷電粒子レンズの
各極子に供給する電気信号をコントロールして前
記ターゲツト上に結像される孔の像の形状を変え
る手段を備えることを特徴としている。
An object of the present invention is to provide a charged particle beam in which the cross-sectional shape of the charged beam irradiated onto a target can be arbitrarily varied without being restricted by the shape of the hole in the mask in the above-mentioned apparatus.
Therefore, the present invention provides a charged particle beam generating means, a mask plate disposed on the charged particle beam path from the generating means and having a hole for shaping the beam cross section, and a first mask plate for forming an image of the hole by the charged particle beam. A charged particle beam device comprising: a charged particle lens; and a second charged particle lens for forming an image of the hole on a target by the charged particle beam formed by the first charged particle lens. , a multipole charged particle lens disposed on the imaging plane of the hole image formed by the first lens; an electric signal supplied to each pole of the multipole charged particle lens is controlled to form the image on the target; It is characterized by comprising means for changing the shape of the hole image.

第1図は本発明の一実施例として示した固定面
積型電子ビーム描画装置の概略図である。図中1
は電子銃で、該電子銃から発生した電子ビーム
は、マスク板2Mに穿たれた正方形状の開口2H
によりその断面が正方形に整形される。3は前記
マスク板2Mの開口面のビーム像を作る為の電子
レンズ、4は該ビーム像5の周囲(即ち、前記電
子レンズ3の像面)に配置された静電型四極子レ
ンズである。該レンズには第2図に示す様に電圧
が印加されている。即ち、静電電極板4a,4b
にはポテンシヨメータ6からの、例えば負電圧が
ゲインAのアンプ7を介して印加され、静電電極
板4c,4dには前記アンプ7の出力がゲイン
(−1)のアンプ8を介して印加される。9は前
記ビーム像5を材料10上に結像する為の電子レ
ンズである。11は中央処理装置(図示せず)か
らの位置指令信号により前記材料10上のビーム
像の結像位置をコントロールする偏向レンズであ
る。
FIG. 1 is a schematic diagram of a fixed area type electron beam lithography apparatus shown as an embodiment of the present invention. 1 in the diagram
is an electron gun, and the electron beam generated from the electron gun is transmitted through a square opening 2H formed in a mask plate 2M.
The cross section is shaped into a square. 3 is an electron lens for forming a beam image of the aperture surface of the mask plate 2M, and 4 is an electrostatic quadrupole lens arranged around the beam image 5 (that is, the image plane of the electron lens 3). . A voltage is applied to the lens as shown in FIG. That is, the electrostatic electrode plates 4a, 4b
For example, a negative voltage from the potentiometer 6 is applied via an amplifier 7 with a gain of A, and the output of the amplifier 7 is applied to the electrostatic electrode plates 4c and 4d via an amplifier 8 with a gain of (-1). applied. Reference numeral 9 denotes an electron lens for forming the beam image 5 onto the material 10. Reference numeral 11 denotes a deflection lens that controls the imaging position of the beam image on the material 10 based on a position command signal from a central processing unit (not shown).

斯くの如き装置において、電子銃1から射出さ
れた電子ビームはマスク板2Mの開口により断面
が正方形状に整形される。該開口を出たビームは
電子レンズ3により静電型四極子レンズ4の大略
中心に結像される。該正方形状のビーム像は、該
四極子レンズにより次の様に長方形状に整形され
る。
In such an apparatus, the electron beam emitted from the electron gun 1 is shaped into a square cross section by the opening of the mask plate 2M. The beam exiting the aperture is imaged by an electron lens 3 approximately at the center of an electrostatic quadrupole lens 4. The square beam image is shaped into a rectangular shape by the quadrupole lens as follows.

該四極子レンズは第2図に示す如きフイールド
を作る。この様なフイールドの中心部に断面が正
方形状のビームが通過しようとすると、矢印に示
す如き電気力線の方向に力を受けてビームの軌道
は変化する。この力は、フイールドの中心、即ち
光軸上では零に等しく、光軸からの距離に大略比
例した強さで働く。即ち、第3図に示す様に、正
方形のビーム像(空間像)は電極板4c,4dか
ら吸引力を受けると同時に電極板4a,4bから
反撥力を受ける。この為、電子レンズ9の絞り面
を通過する像はa′,b′,c′,d′の如き正方形状に
はならず、ABCDの如き長方形状となり、該電
子レンズにより材料10上に結像される像も、
a″,b″,c″,d″の如き正方形状とはならず、A′,
B′,C′,D′の如き長方形状となる。この長方形
の縦横の長さ比は四極子レンズ4の静電電極板に
印加する電圧の強さによりコントロールすること
が出来る。又、静電電極板4a,4bに正の電圧
を4c,4dに負の電圧を夫々印加すれば整形さ
れる像の縦横が逆になる。
The quadrupole lens creates a field as shown in FIG. When a beam with a square cross section attempts to pass through the center of such a field, the trajectory of the beam changes as it receives a force in the direction of the electric lines of force as shown by the arrows. This force is equal to zero at the center of the field, that is, on the optical axis, and acts with a strength roughly proportional to the distance from the optical axis. That is, as shown in FIG. 3, the square beam image (aerial image) receives an attractive force from the electrode plates 4c and 4d, and at the same time receives a repulsive force from the electrode plates 4a and 4b. Therefore, the image passing through the aperture surface of the electron lens 9 does not have a square shape such as a', b', c', d', but a rectangular shape such as ABCD, and is focused on the material 10 by the electron lens. The image that is imaged,
It is not a square shape like a″, b″, c″, d″, but A′,
They will be rectangular shapes like B', C', and D'. The length and width ratio of this rectangle can be controlled by the strength of the voltage applied to the electrostatic electrode plate of the quadrupole lens 4. Further, by applying a positive voltage to the electrostatic electrode plates 4a and 4b and a negative voltage to the electrostatic electrode plates 4c and 4d, the vertical and horizontal directions of the shaped image are reversed.

さて、ここで非常に重要なポイントは、四極子
レンズ4を電子レンズ3の像面に配置したことで
ある。該配置により、第4図に示す様に該電子レ
ンズ3の空間像abcd中の一点から出るビームは
X方向に進むビームもY方向に進むビームも同じ
強さで曲げられるので、材料10上に到達した
時、何れから来たビームも1点で交わる。即ち、
非点収差によるポケを発生しない。尚、9′,1
0′は夫々電子レンズ9の絞り面、材料面である。
Now, the very important point here is that the quadrupole lens 4 is placed on the image plane of the electron lens 3. With this arrangement, as shown in FIG. 4, the beam emitted from one point in the aerial image abcd of the electron lens 3 is bent by the same strength as the beam proceeding in the X direction and the beam proceeding in the Y direction. When they arrive, the beams coming from either direction intersect at one point. That is,
No pockets due to astigmatism occur. Furthermore, 9', 1
0' are the aperture surface and material surface of the electronic lens 9, respectively.

前記例では非点収差によるボケを発生しない
で、正方形ビームを長方形ビームに整形するもの
を示したが、マスク板を光軸に垂直な面で例えば
45゜回転させ、四極子レンズ4a,4b,4c,
4dの中心に第5図の実線に示す如きビーム像を
作れば、材料10上には破線で示す如き菱形の像
が結像される。又、四極子レンズを45゜ずらして
2組設け、電気的にこれらのレンズが作るフイー
ルドを適宜回転させ、材料上に菱形状の像が平行
四辺形状の像を結像させる様にしてもよい。又、
前記実施例では静電型の四極子レンズを例に上げ
たが、電磁型の四極子を使用してもよい。又、四
極子レンズは八極子レンズを重ねて、整形の精度
を上げる様にしてもよい。又、本発明は四極子に
限定されない。例えばスポツト状ビーム(丸型ビ
ーム)を六極子レンズで三角形ビームに整形する
ことも可能である。
In the above example, a square beam is shaped into a rectangular beam without causing blurring due to astigmatism.
Rotate by 45 degrees, and quadrupole lenses 4a, 4b, 4c,
If a beam image as shown by the solid line in FIG. 5 is created at the center of 4d, a diamond-shaped image as shown by the broken line will be formed on the material 10. Alternatively, two sets of quadrupole lenses may be provided, shifted by 45 degrees, and the field formed by these lenses may be electrically rotated appropriately so that a diamond-shaped image forms a parallelogram-shaped image on the material. . or,
In the above embodiments, an electrostatic quadrupole lens was used as an example, but an electromagnetic quadrupole lens may also be used. Further, the quadrupole lens may be stacked with the octupole lens to improve the precision of shaping. Also, the present invention is not limited to quadrupoles. For example, it is also possible to shape a spot beam (round beam) into a triangular beam using a hexapole lens.

本発明によれば、多極子レンズの中心に結像さ
れるビームの断面形状を、該多極子レンズのレン
ズ作用により三角形状、長方形状、菱形状又は平
行四辺形状に、材料上で非点収差によるボケを発
生しないで整形することが出来る。又、他のレン
ズ系で発生する形状変化を多極子レンズで非点収
差によるボケを発生せずに修正できる。
According to the present invention, the cross-sectional shape of the beam imaged at the center of the multipole lens is shaped into a triangle, rectangle, rhombus, or parallelogram by the lens action of the multipole lens, and astigmatism is caused on the material. It is possible to reshape images without causing blurring. In addition, shape changes that occur in other lens systems can be corrected using a multipole lens without causing blurring due to astigmatism.

【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を示した固定面積型
電子ビーム描画装置の概略図、第2図〜第4図は
該装置の動作の説明を補促する為に用いた図、第
5図は四極子レンズの中心に出来るビーム像を第
3図に示す実施例に対し、45゜回転させた時に材
料上に結像されるビーム像の形状を示すものであ
る。 1……電子銃、3……電子レンズ、4……静電
型四極子レンズ、5……ビーム像、9……電子レ
ンズ、10……材料。
FIG. 1 is a schematic diagram of a fixed area electron beam lithography system showing an embodiment of the present invention, FIGS. 2 to 4 are diagrams used to assist in explaining the operation of the system, and FIG. The figure shows the shape of the beam image formed on the material when the beam image formed at the center of the quadrupole lens is rotated by 45 degrees with respect to the embodiment shown in FIG. 1... Electron gun, 3... Electron lens, 4... Electrostatic quadrupole lens, 5... Beam image, 9... Electron lens, 10... Material.

Claims (1)

【特許請求の範囲】[Claims] 1 荷電粒子ビーム発生手段、該発生手段からの
荷電粒子ビーム通路上に配置されビーム断面整形
用の孔を有するマスク板、荷電粒子ビームによる
孔の像を結像させるための第1の荷電粒子レン
ズ、該第1の荷電粒子レンズによつて結像された
荷電粒子ビームによる前記孔の像をターゲツト上
に結像する為の第2の荷電粒子レンズを備えた荷
電粒子ビーム装置において、前記第1のレンズに
よる孔の像の結像面に配置された多極子荷電粒子
レンズ、該多極子荷電粒子レンズの各極子に供給
する電気信号をコントロールして前記ターゲツト
上に結像される孔の像の形状を変える手段を備え
る荷電粒子ビーム装置。
1. Charged particle beam generating means, a mask plate disposed on the charged particle beam path from the generating means and having a hole for shaping the beam cross section, and a first charged particle lens for forming an image of the hole by the charged particle beam. , a charged particle beam device comprising a second charged particle lens for forming an image of the hole by the charged particle beam imaged by the first charged particle lens on a target; a multipole charged particle lens disposed on the imaging plane of the hole image formed by the lens; controlling electric signals supplied to each pole of the multipole charged particle lens to form an image of the hole on the target; Charged particle beam device with means for changing shape.
JP59112469A 1984-06-01 1984-06-01 Charged particle beam apparatus Granted JPS60257053A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59112469A JPS60257053A (en) 1984-06-01 1984-06-01 Charged particle beam apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59112469A JPS60257053A (en) 1984-06-01 1984-06-01 Charged particle beam apparatus

Publications (2)

Publication Number Publication Date
JPS60257053A JPS60257053A (en) 1985-12-18
JPH039581B2 true JPH039581B2 (en) 1991-02-08

Family

ID=14587417

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59112469A Granted JPS60257053A (en) 1984-06-01 1984-06-01 Charged particle beam apparatus

Country Status (1)

Country Link
JP (1) JPS60257053A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR102123887B1 (en) * 2016-07-14 2020-06-17 주식회사 히타치하이테크 Ion milling device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5835852A (en) * 1981-08-28 1983-03-02 Agency Of Ind Science & Technol Lens for charged beam

Also Published As

Publication number Publication date
JPS60257053A (en) 1985-12-18

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