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JP3603779B2 - Electron detection device, charged particle beam device, semiconductor integrated circuit device, and processing, observation, and inspection method of the semiconductor integrated circuit device - Google Patents
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JP3603779B2 - Electron detection device, charged particle beam device, semiconductor integrated circuit device, and processing, observation, and inspection method of the semiconductor integrated circuit device - Google Patents

Electron detection device, charged particle beam device, semiconductor integrated circuit device, and processing, observation, and inspection method of the semiconductor integrated circuit device Download PDF

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JP3603779B2
JP3603779B2 JP2000339137A JP2000339137A JP3603779B2 JP 3603779 B2 JP3603779 B2 JP 3603779B2 JP 2000339137 A JP2000339137 A JP 2000339137A JP 2000339137 A JP2000339137 A JP 2000339137A JP 3603779 B2 JP3603779 B2 JP 3603779B2
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electrons
spatula
charged particle
detector
particle beam
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JP2002141013A (en
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優臣 田中
正己 勝山
枢容 浅井
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Hitachi Ltd
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Hitachi Ltd
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Description

【0001】
【発明の属する技術分野】
本発明は、荷電粒子ビーム装置に装備される反射電子や二次電子などを検出する電子検出装置,半導体集積回路装置などの観察,検査に用いられる荷電粒子ビーム装置,荷電粒子ビーム装置を用いて加工,観察,検査される半導体集積回路装置、または半導体集積回路装置の加工,観察,検査方法に関する。
【0002】
【従来の技術】
走査型電子顕微鏡や収束イオンビーム装置,電子ビーム描画装置に代表される荷電粒子ビーム装置は電子ビームやイオンビームを試料上に照射して観察,加工,描画を行う装置である。このうち半導体集積回路装置の製造,検査に用いられる電子ビーム描画装置,測長用走査型電子顕微鏡,走査型電子顕微鏡を応用した検査装置などは、対象とする素子の寸法が年々微細になり、その結果、各装置に要求される電子ビームの位置精度が高くなっている。電子ビーム描画装置では、試料であるウェハの位置測定のために、ウェハを保持するパレット上のマークに電子ビームを照射し、電子検出装置を用いてマークからの反射電子や二次電子を信号処理してマークの位置を測定している。また、走査電子顕微鏡では、試料に電子ビームを照射し、電子検出装置を用いて試料からの反射電子や二次電子を信号処理して試料の画像を得る。電子検出装置は、電子を検出する検出器と、検出器を保持するホルダとからなる。ホルダは検出器を保持するだけでなく、電子を検出器へ導く開口に相当する構造も併せ持つ。ホルダの構造によっては、検出器で得られた信号は、試料から直接飛来した反射電子や二次電子のみに限らず、反射電子などがホルダの開口以外の部位に当たり二次反射電子などとなり、二次反射電子などが試料に再度当たり三次反射電子などとなり検出器で検出される誤信号なども含まれる。これら高次の反射電子などを検出することに因る誤信号が、走査電子顕微鏡においては画像処理精度の低下、電子ビーム描画装置においては位置精度の低下をまねいている。また、高次の反射電子などに起因する誤信号により、画像処理精度や位置精度の向上が阻まれることで、素子寸法の微細化の進歩を緩慢なものとしている。
【0003】
この高次の反射電子などが検出器へ導入されることを低減する手段として、例えば、電子を導入する開口以外のホルダ表面を回折格子状にして反射電子を散乱する方法が提案されている。反射電子を散乱することで検出器に試料から飛来する三次の反射電子などのもととなる二次の反射電子は低減されるが、三次以上の高次の反射電子などが低減される訳ではないので、誤信号の低減に大きな効果は期待できない。
【0004】
遠距離感光作用低減することを目的として、例えば、特開昭61−19126号公報に記載のように、試料の対向壁面に凹凸を設け、反射電子を散乱させることで、二次の反射電子が試料へ再入射することを防止する方法が提案されている。この様な方法により、試料の対向壁面からの二次の反射電子は低減されるが、凹凸で散乱された高次の反射電子は、対向壁面より上方へ飛散することはできず、結局対向壁面から試料へ戻ってくるため、高次の反射電子などの低減に大きな効果は期待できない。
【0005】
また、遠距離感光作用とビームドリフトとを低減することを目的として、例えば、特開2000−2960413号公報に記載のように、斜めハニカム開孔構造とした反射防止機構を、試料と試料上方の構造物との間に配置し、反射電子が二次の反射電子として試料へ再入射することを防止する方法が提案されている。この様な方法により、試料上方の構造物からの二次の反射電子は低減されるが、反射防止機構が板体であるために開孔の残り部分の面積が大きく、開孔の残り部分に当たった反射電子に起因する三次以上の高次の反射電子などの低減に大きな効果は期待できない。
【0006】
【発明が解決しようとする課題】
本発明は、反射電子などの検出精度を低下させる高次の反射電子や高次の二次電子に起因する誤信号を低減することを目的とする。
【0007】
また、電子検出装置の誤信号の低減により、安定して高精度で、加工,観察,検査され、素子寸法が微細化された半導体集積回路装置、その加工,観察,検査方法を提供することを目的とする。
【0008】
【課題を解決するための手段】
本発明の実施態様において、電子を検出する検出器と検出器を担持するホルダとを具備し、荷電粒子ビームを試料上に照射し試料からの反射電子もしくは二次電子を検出する場合において、ホルダをへら絞り部を備える複数の筒で構成する。へら絞り部は延長線が荷電粒子ビームの中心軸と試料との交点に交差する構造とする。へら絞り部は、荷電粒子ビームの中心軸を基準にして採取角度範囲の内にある反射電子もしくは二次電子を選択的に検出器へ導入する角度とし、これらへら絞り部を備える筒の間に検出器を配置する。採取角度範囲の外にある反射電子もしくは二次電子が高次の反射電子もしくは高次の二次電子となることを防ぐ為に、採取角度範囲の外にある反射電子もしくは二次電子を選択的に捕獲するへら絞り部を備える筒を、採取角度範囲の内にある反射電子もしくは二次電子を選択的に検出器へ導入する角度としたへら絞り部を備える筒の内外に配置する。各へら絞り部の先端は、へら絞り部の先端に当たる反射電子や二次電子が二次反射電子や二次電子となっても、検出器へ導入されない位置関係とする。採取角度範囲の内にある反射電子もしくは二次電子を選択的に検出器へ導入し、採取角度範囲の外にある反射電子もしくは二次電子を選択的に捕獲することで、高次の反射電子や高次の二次電子に起因する誤信号が低減され、反射電子もしくは二次電子の検出精度を向上することができる。
【0009】
【発明の実施の形態】
以下、本発明の実施例を、図面を用いて説明する。
(実施例1)
図1は本発明の第1の実施例が適用される電子ビーム描画装置の構成を示す略縦断面図、図2は従来の技術において電子検出装置の構造を示す縦断面図、図3は本発明の第1の実施例において電子検出装置の構造を示す縦断面図である。本実施例では、電子ビーム描画装置を一例として説明するが、他の荷電粒子ビーム装置において本実施例を適用することは容易である。
【0010】
図1に示した電子ビーム描画装置において、電子銃1から放出された電子ビーム17は絞り2で円形に成形され、絞り5上に照射され、レンズ9にて絞り8上に結像される。この絞り8上の像はレンズ10で投影され、絞り11を通過してレンズ14に入る。さらにレンズ14と偏向器13で投影偏向されて、感光剤の塗布された試料18上に投影され描画を行う。このとき絞り8にあらかじめ設けてあるパターン形状の開口を、偏向器7により選択する。偏向器13で偏向可能な領域以外は、ステージ19を移動させて描画を行う。位置あわせのために試料上に配置されたマーク28からの反射電子29などを電子検出装置の検出器15で検出し、ステージ19の位置をレーザ測長器26からの信号で計測する。
【0011】
図2に示すように従来の技術を用いたホルダ30の形状では、反射電子31などを検出器32へ導入する開口33以外のホルダ表面に当たった反射電子34などによる高次の反射電子35,36などが、検出器32へ飛来して誤信号を増加させる。このことが信号処理の精度を落とす原因の一つになっている。また、ホルダ底部へ当たった反射電子37などによる高次の反射電子38が試料39に影響することもある。
【0012】
この課題に対する本発明での解決手段を以下に述べる。ここで、図3に示すように、ホルダはへら絞り部を備えた複数の筒41,42,43,44により構成される。所望の採取角度範囲45のへら絞り部46,47を持つ筒42,43の間に検出器49を配置する。検出器49を挟む筒42,43のへら絞り部46,47は、試料50から直接飛来する反射電子51などのみ選択的に導入する。採取角度範囲45の外の筒41もしくはへら絞り部48は、試料50から飛来した反射電子52,53などが高次の反射電子などとならない様に捕獲し、これら筒41もしくはへら絞り部48の先端に当たった反射電子54,55などによる高次の反射電子56,57,58などをも捕獲し、検出器49へ導入されるのを防ぐ。さらに最外の筒のへら絞り部より外側へ飛行する反射電子64などは、へら絞り部に当たることがないので高次の反射電子などとならず、試料50へ入射して影響することもない。筒41,42,43,44もしくはへら絞り部46,
47,48の先端の位置関係は、最内の筒41とこの筒41の先端に当たる反射電子54の軌跡59との角度60を最内の筒41を軸対称とした直線62上に検出器49を挟む内側の筒42のへら絞り部46の先端が配置されるようにし、検出器49を挟む外側の筒43のへら絞り部47の先端と採取角度範囲45の外のへら絞り部48の先端を結ぶ直線63は試料50に平行とする。これにより、高次の反射電子などに起因する誤信号を低減することが可能となる。
(実施例2)
図4は本発明の第2の実施例において電子検出装置の構造を示す縦断面図である。上記第1の実施例と同様に描画動作を行う。ここで、図4に示すように、ホルダはへら絞り部を備えた複数の筒66,67,68,69により構成される。所望の採取角度範囲70のへら絞り部71,72を持つ筒67,68の間に検出器74を配置する。検出器74を挟む筒67,68のへら絞り部71,72は、試料75から直接飛来する反射電子76などのみ選択的に導入する。採取角度範囲70の外の筒66もしくはへら絞り部73は、試料75から飛来した反射電子77,78などが高次の反射電子などとならない様に捕獲し、これら筒66もしくはへら絞り部73の先端に当たった反射電子79などによる高次の反射電子
80などをも捕獲し、検出器74へ導入されるのを防ぐ。さらに最外の筒69のへら絞り部73より外側へ飛行する反射電子81などは、へら絞り部に当たることがないので高次の反射電子などとならず、試料75へ入射して影響することもない。筒66,67,68,69もしくはへら絞り部71,72,73の先端の位置関係は、最内の筒66を延長した直線82上に検出器74を挟む内側の筒
67のへら絞り部71の先端が配置されるようにし、検出器74を挟む外側の筒68のへら絞り部72の先端と採取角度範囲70の外のへら絞り部73の先端を結ぶ直線83は試料75に平行とする。これにより、高次の反射電子などに起因する誤信号を低減することが可能となる。
(実施例3)
以上の実施例は電子ビーム描画装置を示したが、本発明の電子検出装置は走査型電子顕微鏡や、走査型電子顕微鏡を応用した検査装置にも容易に適用可能である。また、電子銃をイオン銃に、電子ビームをイオンビームに、試料からの反射電子を二次電子に置きかえれば収束イオンビーム装置にも適用可能である。このときイオンビームに関してもレンズや絞り、その他の機構は電子ビーム装置の場合と同じ機能をもつ。
(実施例4)
本発明の電子検出装置を備えた電子ビーム描画装置を使用した電子ビーム描画方法を用いた半導体集積回路の製造工程を述べる。
【0013】
Nマイナスシリコン基板に通常の方法でPウエル層,P層,フィールド酸化膜,多結晶シリコン/シリコン酸化膜ゲート,P高濃度拡散層,N高濃度拡散層、などを形成する。次に、リンガラス(PSG)の絶縁膜を被着し、絶縁膜をドライエッチングしてコンタクトホールを形成する。
【0014】
次に、通常の方法でW/TiN電極配線材を被着し、その上に感光剤を塗布し、本発明の電子ビーム描画方法を用いて感光剤のパターンニングを行う。そして、ドライエッチングなどによりW/TiN電極配線を形成する。
【0015】
次に層間絶縁膜を形成し、通常の方法でホールパターンを形成した。ホールパターンの中はWプラグで埋め込み、Al配線もしくはCu配線を連結する。以降のパッシベーション工程は従来法を用いる。
【0016】
なお、本実施例では主な製造工程のみを説明したが、W/TiN電極配線形成のリソグラフィ工程で本発明の電子ビーム描画方法を用いたこと以外は従来法と同じ工程を用いた。以上の工程により、質が低下することなく微細パターンを形成することができ、CMOSLSIを高歩留まりで製造することが出来た。本発明の電子ビーム描画装置を用い半導体集積回路を製作した結果、マーク検出精度が向上したことにより歩留まりが向上し、生産量を増加することができた。
【0017】
【発明の効果】
以上述べたように、本発明によれば、反射電子などの検出精度を低下させる高次の反射電子や高次の二次電子に起因する誤信号を低減することができる。
【0018】
また、電子検出装置の誤信号の低減により、安定して高精度で、加工,観察,検査され、素子寸法が微細化された半導体集積回路装置、その加工,観察,検査方法を提供することができる。
【図面の簡単な説明】
【図1】本発明の第1の実施例が適用される電子ビーム描画装置の構成を示す略縦断面図。
【図2】従来の技術において電子検出装置の構造を示す縦断面図。
【図3】本発明の第1の実施例において電子検出装置の構造を示す縦断面図。
【図4】本発明の第1の実施例において電子検出装置の構造を示す縦断面図。
【符号の説明】
12,30…ホルダ、15,32,49,74…検出器、17…電子ビーム、18,39,50,75…試料、19…ステージ、23…制御用コンピュータ、28…マーク、29,31,34,37,51,52,53,54,55,64,76,77,78,79,81…反射電子、33…開口、35,38,56,58,80…二次反射電子、36,57…三次反射電子、41,42,43,
44,66,67,68,69…筒、45…採取角度範囲、46,47,48,71,72,73…へら絞り部、59…軌跡、60…角度。
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention uses a charged particle beam device, a charged particle beam device used for observation and inspection of a semiconductor integrated circuit device and the like, which is provided in the charged particle beam device and detects reflected electrons and secondary electrons. The present invention relates to a semiconductor integrated circuit device to be processed, observed, and inspected, or a method of processing, observing, and inspecting a semiconductor integrated circuit device.
[0002]
[Prior art]
BACKGROUND ART A charged particle beam device represented by a scanning electron microscope, a focused ion beam device, and an electron beam drawing device is a device that performs observation, processing, and drawing by irradiating a sample with an electron beam or an ion beam. Among them, electron beam lithography systems used in the manufacture and inspection of semiconductor integrated circuit devices, scanning electron microscopes for length measurement, and inspection systems that use scanning electron microscopes, etc., have smaller and smaller element sizes year by year. As a result, the position accuracy of the electron beam required for each device is increased. An electron beam lithography system irradiates a mark on a pallet holding a wafer with an electron beam to measure the position of a sample wafer, and uses an electron detector to process reflected electrons and secondary electrons from the mark. The position of the mark is measured. In a scanning electron microscope, a sample is irradiated with an electron beam, and an electron detector is used to process reflected electrons and secondary electrons from the sample, thereby obtaining an image of the sample. The electron detection device includes a detector that detects electrons and a holder that holds the detector. The holder not only holds the detector, but also has a structure corresponding to an opening for guiding electrons to the detector. Depending on the structure of the holder, the signal obtained by the detector is not limited to the reflected electrons and secondary electrons directly flying from the sample, but the reflected electrons and the like hit the parts other than the opening of the holder and become secondary reflected electrons. Secondary reflected electrons and the like again strike the sample, become tertiary reflected electrons, and include erroneous signals detected by the detector. These erroneous signals resulting from the detection of higher-order reflected electrons and the like lead to a decrease in image processing accuracy in a scanning electron microscope and a decrease in position accuracy in an electron beam writing apparatus. In addition, erroneous signals caused by higher-order reflected electrons and the like hinder improvements in image processing accuracy and positional accuracy, thereby slowing progress in miniaturization of element dimensions.
[0003]
As means for reducing the introduction of higher-order reflected electrons and the like into the detector, for example, a method has been proposed in which the surface of the holder other than the opening for introducing electrons is made into a diffraction grating shape to scatter reflected electrons. By scattering backscattered electrons, secondary backscattered electrons, which are the source of tertiary backscattered electrons that fly from the sample to the detector, are reduced, but tertiary or higher-order backscattered electrons are not reduced. Since there is no such effect, a great effect cannot be expected in reducing false signals.
[0004]
For the purpose of reducing the long-range photosensitive action, for example, as described in JP-A-61-19126, unevenness is provided on the opposite wall surface of the sample to scatter reflected electrons, so that secondary reflected electrons are generated. A method has been proposed to prevent re-incident on the sample. By such a method, secondary reflected electrons from the opposed wall surface of the sample are reduced, but higher-order reflected electrons scattered by the unevenness cannot be scattered above the opposed wall surface, and eventually the opposed wall surface is not scattered. Since it returns from the sample to the sample, a large effect cannot be expected in reducing high-order reflected electrons and the like.
[0005]
Further, for the purpose of reducing the long-distance photosensitive action and the beam drift, for example, as described in Japanese Patent Application Laid-Open No. 2000-2960413, an anti-reflection mechanism having an oblique honeycomb opening structure is provided on the sample and above the sample. There has been proposed a method of disposing between a structure and a structure to prevent reflected electrons from re-entering the sample as secondary reflected electrons. By such a method, secondary reflected electrons from the structure above the sample are reduced, but since the antireflection mechanism is a plate, the area of the remaining portion of the opening is large, and the remaining portion of the opening is large. No significant effect can be expected in reducing the third-order or higher-order backscattered electrons caused by the backscattered electrons.
[0006]
[Problems to be solved by the invention]
An object of the present invention is to reduce erroneous signals caused by higher-order reflected electrons and higher-order secondary electrons that lower the detection accuracy of reflected electrons and the like.
[0007]
It is another object of the present invention to provide a semiconductor integrated circuit device which has been processed, observed, and inspected stably and with high precision by reducing the number of erroneous signals of the electron detection device, and has a finer element size, and a method of processing, observing and inspecting the same. Aim.
[0008]
[Means for Solving the Problems]
In an embodiment of the present invention, a detector for detecting electrons and a holder for holding the detector are provided, and when a charged particle beam is irradiated onto the sample to detect reflected electrons or secondary electrons from the sample, the holder Is composed of a plurality of cylinders having a spatula section. The spatula section has a structure in which the extension line intersects the intersection between the central axis of the charged particle beam and the sample. The spatula section has an angle for selectively introducing reflected electrons or secondary electrons within the sampling angle range with respect to the central axis of the charged particle beam to the detector, and between the cylinders having these spatula sections. Position the detector. To prevent reflected or secondary electrons outside the sampling angle range from becoming higher-order reflected or higher-order secondary electrons, selectively use reflected or secondary electrons outside the sampling angle range. The tube provided with the spatula restricting portion is disposed inside and outside the tube provided with the spatula restricting portion at an angle for selectively introducing reflected electrons or secondary electrons within the sampling angle range to the detector. Even if the reflected electrons or secondary electrons hitting the tip of the spatula are turned into secondary reflected electrons or secondary electrons, the tips of the spatula stops are not introduced into the detector. By selectively introducing reflected electrons or secondary electrons within the sampling angle range to the detector and selectively capturing reflected electrons or secondary electrons outside the sampling angle range, higher-order reflected electrons can be obtained. The erroneous signal caused by the high-order secondary electrons is reduced, and the detection accuracy of the reflected electrons or the secondary electrons can be improved.
[0009]
BEST MODE FOR CARRYING OUT THE INVENTION
Hereinafter, embodiments of the present invention will be described with reference to the drawings.
(Example 1)
FIG. 1 is a schematic longitudinal sectional view showing the structure of an electron beam writing apparatus to which the first embodiment of the present invention is applied, FIG. 2 is a longitudinal sectional view showing the structure of an electron detecting apparatus in the prior art, and FIG. It is a longitudinal section showing the structure of the electronic detection device in a 1st example of the present invention. In this embodiment, an electron beam lithography apparatus will be described as an example. However, it is easy to apply this embodiment to another charged particle beam apparatus.
[0010]
In the electron beam drawing apparatus shown in FIG. 1, the electron beam 17 emitted from the electron gun 1 is formed into a circular shape by the stop 2, irradiated on the stop 5, and imaged on the stop 8 by the lens 9. The image on the stop 8 is projected by the lens 10, passes through the stop 11, and enters the lens 14. Further, the light is projected and deflected by the lens 14 and the deflector 13, and is projected and drawn on the sample 18 coated with the photosensitive agent. At this time, a pattern-shaped opening provided in advance in the stop 8 is selected by the deflector 7. The drawing is performed by moving the stage 19 except for the area where the deflector 13 can deflect. The reflected electrons 29 from the mark 28 placed on the sample for alignment are detected by the detector 15 of the electron detection device, and the position of the stage 19 is measured by a signal from the laser length measuring device 26.
[0011]
As shown in FIG. 2, in the shape of the holder 30 using the conventional technique, higher-order reflected electrons 35 due to reflected electrons 34 and the like hitting the holder surface other than the opening 33 for introducing the reflected electrons 31 and the like into the detector 32, 36 and the like fly to the detector 32 and increase the number of false signals. This is one of the causes for lowering the accuracy of signal processing. Also, higher-order reflected electrons 38 such as reflected electrons 37 hitting the bottom of the holder may affect the sample 39.
[0012]
The means for solving this problem in the present invention will be described below. Here, as shown in FIG. 3, the holder is composed of a plurality of cylinders 41, 42, 43, 44 provided with a spatula. A detector 49 is arranged between the cylinders 42 and 43 having the spatula sections 46 and 47 in a desired sampling angle range 45. The spatula portions 46 and 47 of the cylinders 42 and 43 sandwiching the detector 49 selectively introduce only the backscattered electrons 51 directly flying from the sample 50. The tube 41 or the spatula portion 48 outside the sampling angle range 45 captures the reflected electrons 52 and 53 flying from the sample 50 so as not to become higher-order reflected electrons, and the like. Higher order backscattered electrons 56, 57, 58, etc. due to backscattered electrons 54, 55, etc. hitting the tip are also captured and prevented from being introduced into the detector 49. Furthermore, the backscattered electrons 64 and the like flying outside the spatula of the outermost tube do not hit the spatula, so they do not become higher-order backscattered electrons and do not enter the sample 50 and affect them. Cylinder 41, 42, 43, 44 or spatula narrowing section 46,
The positional relationship between the tips of 47 and 48 is such that the angle 60 between the innermost cylinder 41 and the trajectory 59 of the reflected electrons 54 hitting the tip of this cylinder 41 is on a straight line 62 with the innermost cylinder 41 being axially symmetric. The tip of the spatula narrowing portion 46 of the inner cylinder 42 sandwiching the detector is arranged, and the tip of the spatula narrowing portion 47 of the outer cylinder 43 sandwiching the detector 49 and the tip of the spatula narrowing portion 48 outside the sampling angle range 45. Is assumed to be parallel to the sample 50. This makes it possible to reduce erroneous signals due to higher-order reflected electrons and the like.
(Example 2)
FIG. 4 is a longitudinal sectional view showing the structure of the electron detection device according to the second embodiment of the present invention. The drawing operation is performed in the same manner as in the first embodiment. Here, as shown in FIG. 4, the holder is composed of a plurality of cylinders 66, 67, 68, 69 each having a spatula. A detector 74 is arranged between cylinders 67 and 68 having spatula portions 71 and 72 in a desired sampling angle range 70. The spatula restricting portions 71 and 72 of the cylinders 67 and 68 sandwiching the detector 74 selectively introduce only the backscattered electrons 76 directly flying from the sample 75. The tube 66 or the spatula 73 outside the sampling angle range 70 captures reflected electrons 77 and 78 flying from the sample 75 so as not to become higher-order reflected electrons and the like. Higher order backscattered electrons 80 and the like due to backscattered electrons 79 and the like striking the tip are also captured, and are prevented from being introduced into the detector 74. Further, the backscattered electrons 81 and the like flying outside the spatula 73 of the outermost cylinder 69 do not hit the spatula, so that they do not become higher-order backscattered electrons or the like, and may be incident on the sample 75 and affect them. Absent. The positional relationship between the ends of the cylinders 66, 67, 68, 69 or the spatula constrictions 71, 72, 73 is determined by the spatula constriction 71 of the inner cylinder 67 sandwiching the detector 74 on a straight line 82 extending the innermost cylinder 66. The straight line 83 connecting the tip of the spatula stop 72 of the outer tube 68 sandwiching the detector 74 and the tip of the spatula stop 73 outside the sampling angle range 70 is parallel to the sample 75. . This makes it possible to reduce erroneous signals due to higher-order reflected electrons and the like.
(Example 3)
Although the above embodiment has shown the electron beam writing apparatus, the electron detection apparatus of the present invention can be easily applied to a scanning electron microscope and an inspection apparatus to which the scanning electron microscope is applied. Further, if the electron gun is replaced with an ion gun, the electron beam is replaced with an ion beam, and the reflected electrons from the sample are replaced with secondary electrons, the present invention can be applied to a focused ion beam apparatus. At this time, the lens, aperture, and other mechanisms of the ion beam have the same functions as those of the electron beam device.
(Example 4)
A manufacturing process of a semiconductor integrated circuit using an electron beam drawing method using an electron beam drawing device provided with the electron detection device of the present invention will be described.
[0013]
A P well layer, a P layer, a field oxide film, a polycrystalline silicon / silicon oxide film gate, a P high concentration diffusion layer, an N high concentration diffusion layer, and the like are formed on an N minus silicon substrate by a usual method. Next, an insulating film of phosphor glass (PSG) is applied, and the insulating film is dry-etched to form a contact hole.
[0014]
Next, a W / TiN electrode wiring material is applied by a usual method, a photosensitive agent is applied thereon, and the photosensitive agent is patterned by using the electron beam drawing method of the present invention. Then, W / TiN electrode wiring is formed by dry etching or the like.
[0015]
Next, an interlayer insulating film was formed, and a hole pattern was formed by a usual method. The hole pattern is buried with a W plug to connect an Al wiring or a Cu wiring. The subsequent passivation process uses a conventional method.
[0016]
In this example, only the main manufacturing process was described, but the same process as the conventional method was used except that the electron beam drawing method of the present invention was used in the lithography process for forming the W / TiN electrode wiring. Through the above steps, a fine pattern can be formed without lowering the quality, and a CMOS LSI can be manufactured with a high yield. As a result of manufacturing a semiconductor integrated circuit using the electron beam lithography apparatus of the present invention, the yield was improved due to the improved mark detection accuracy, and the production amount could be increased.
[0017]
【The invention's effect】
As described above, according to the present invention, it is possible to reduce erroneous signals caused by higher-order reflected electrons and higher-order secondary electrons that lower the detection accuracy of reflected electrons and the like.
[0018]
Further, it is possible to provide a semiconductor integrated circuit device which has been processed, observed, and inspected stably and with high precision by reducing the erroneous signal of the electron detection device, and has a fine element size, and a method of processing, observing and inspecting the same. it can.
[Brief description of the drawings]
FIG. 1 is a schematic longitudinal sectional view showing a configuration of an electron beam writing apparatus to which a first embodiment of the present invention is applied.
FIG. 2 is a longitudinal sectional view showing the structure of an electron detection device in a conventional technique.
FIG. 3 is a longitudinal sectional view showing the structure of an electron detection device according to the first embodiment of the present invention.
FIG. 4 is a longitudinal sectional view showing the structure of an electron detection device according to the first embodiment of the present invention.
[Explanation of symbols]
12, 30, holder, 15, 32, 49, 74 detector, 17 electron beam, 18, 39, 50, 75 sample, 19 stage, 23 control computer, 28 mark, 29, 31, 34, 37, 51, 52, 53, 54, 55, 64, 76, 77, 78, 79, 81: reflected electrons, 33: aperture, 35, 38, 56, 58, 80: secondary reflected electrons, 36, 57 tertiary backscattered electrons, 41, 42, 43,
44, 66, 67, 68, 69 ... cylinder, 45 ... sampling angle range, 46, 47, 48, 71, 72, 73 ... spatula narrowing section, 59 ... locus, 60 ... angle.

Claims (3)

電子を検出する検出器と前記検出器を担持するホルダとを具備し、荷電粒子ビームを試料上に照射し該試料からの反射電子もしくは二次電子を検出する電子検出装置において、前記ホルダがへら絞り部を備える複数の筒で構成され、前記へら絞り部は延長線が前記荷電粒子ビームの中心軸と該試料との交点に交差し、前記へら絞り部のうち前記中心軸を基準にして採取角度範囲の内にある反射電子もしくは二次電子を選択的に導入するへら絞り部を備える筒の間に前記検出器が配置され、前記へら絞り部のうち前記採取角度範囲の外にある反射電子もしくは二次電子を選択的に捕獲するへら絞り部を備える筒を備えることを特徴とする電子検出装置。An electron detection device, comprising: a detector for detecting electrons; and a holder for holding the detector, wherein the holder is a spatula in an electron detection device that irradiates a charged particle beam onto a sample and detects reflected electrons or secondary electrons from the sample. It is composed of a plurality of cylinders having an aperture portion, and the spatula aperture portion has an extension line intersecting the intersection of the center axis of the charged particle beam and the sample, and is sampled based on the central axis of the spatula aperture portion. The detector is arranged between a cylinder having a spatula section for selectively introducing reflected electrons or secondary electrons within an angle range, and the reflected electrons outside the sampling angle range of the spatula section. Alternatively, there is provided an electron detection device including a cylinder provided with a spatula section for selectively capturing secondary electrons. 荷電粒子ビームを発生する荷電粒子源と、前記荷電粒子ビームを偏向する偏向器と、前記荷電粒子ビームの形状を制限する孔を備えた絞りとを具備し、前記荷電粒子ビームを試料上に照射し、該試料からの反射電子もしくは二次電子を検出する電子検出装置を備え、該試料を観察,加工、または描画を行う荷電粒子ビーム装置において、電子を検出する検出器と前記検出器を担持するホルダとを具備し、前記ホルダがへら絞り部を備える複数の筒で構成され、前記へら絞り部は延長線が前記荷電粒子ビームの中心軸と該試料との交点に交差し、前記中心軸を基準にして採取角度範囲の内にある反射電子もしくは二次電子を選択的に導入するへら絞り部を備える筒の間に前記検出器が配置され、前記採取角度範囲の外にある反射電子もしくは二次電子を選択的に捕獲するへら絞り部を備える筒を備えたことを特徴とする荷電粒子ビーム装置。A charged particle source for generating a charged particle beam, a deflector for deflecting the charged particle beam, and a diaphragm having a hole for limiting the shape of the charged particle beam, and irradiating the sample with the charged particle beam. A charged particle beam apparatus for observing, processing, or drawing the sample, comprising a detector for detecting electrons and a detector for detecting reflected electrons or secondary electrons from the sample; And a holder comprising a plurality of cylinders having a spatula section, wherein the spatula diaphragm section has an extension line intersecting the intersection of the center axis of the charged particle beam and the sample, and the central axis The detector is arranged between a cylinder having a spatula section for selectively introducing reflected electrons or secondary electrons within the sampling angle range with reference to the reflected electrons or outside the sampling angle range. two A charged particle beam apparatus characterized by comprising a cylinder with a spatula throttle portion for selectively captures electrons. 電子を検出する検出器と前記検出器を担持するホルダとを具備し、前記ホルダがへら絞り部を備える複数の筒で構成され、前記へら絞り部は延長線が前記荷電粒子ビームの中心軸と該試料との交点に交差し、前記中心軸を基準にして採取角度範囲の内にある反射電子もしくは二次電子を選択的に導入するへら絞り部を備える筒の間に前記検出器が配置され、前記採取角度範囲の外にある反射電子もしくは二次電子を選択的に捕獲するへら絞り部を備える筒を備えた荷電粒子ビーム装置により電子を照射されて加工され、発生した反射電子もしくは二次電子を検出されて、観察、または検査されることを特徴とする半導体集積回路装置の加工,観察,検査方法。It comprises a detector for detecting electrons and a holder for carrying the detector, wherein the holder comprises a plurality of cylinders provided with a spatula, and the spatula is a central axis of the charged particle beam having an extended line extending therefrom. The detector intersects the intersection with the sample, and the detector is disposed between a cylinder having a spatula section for selectively introducing reflected electrons or secondary electrons within the sampling angle range with respect to the central axis. Electrons are irradiated and processed by a charged particle beam apparatus having a cylinder provided with a spatula section for selectively capturing reflected electrons or secondary electrons outside the sampling angle range, and the generated reflected electrons or secondary electrons are generated. A method of processing, observing, and inspecting a semiconductor integrated circuit device, wherein electrons are detected, observed, or inspected.
JP2000339137A 2000-11-01 2000-11-01 Electron detection device, charged particle beam device, semiconductor integrated circuit device, and processing, observation, and inspection method of the semiconductor integrated circuit device Expired - Fee Related JP3603779B2 (en)

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