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JPH0252828B2 - - Google Patents
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JPH0252828B2 - - Google Patents

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Publication number
JPH0252828B2
JPH0252828B2 JP56047106A JP4710681A JPH0252828B2 JP H0252828 B2 JPH0252828 B2 JP H0252828B2 JP 56047106 A JP56047106 A JP 56047106A JP 4710681 A JP4710681 A JP 4710681A JP H0252828 B2 JPH0252828 B2 JP H0252828B2
Authority
JP
Japan
Prior art keywords
electrode
electron beam
voltage
deceleration
secondary electrons
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
Application number
JP56047106A
Other languages
Japanese (ja)
Other versions
JPS57161556A (en
Inventor
Akio Ito
Yoshiaki 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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP56047106A priority Critical patent/JPS57161556A/en
Publication of JPS57161556A publication Critical patent/JPS57161556A/en
Publication of JPH0252828B2 publication Critical patent/JPH0252828B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R31/00Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
    • G01R31/28Testing of electronic circuits, e.g. by signal tracer
    • G01R31/302Contactless testing
    • G01R31/305Contactless testing using electron beams

Landscapes

  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Current Or Voltage (AREA)
  • Tests Of Electronic Circuits (AREA)

Description

【発明の詳細な説明】 本発明は、電子ビームによる電圧測定装置に関
する。特に、二次電子の有する運動エネルギーが
電子ビームの照射を受ける試料の電位に依存する
性質を利用してなす電子ビームによる電圧測定装
置の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a voltage measuring device using an electron beam. In particular, the present invention relates to improvements in voltage measuring devices using electron beams that utilize the property that the kinetic energy of secondary electrons depends on the potential of a sample irradiated with the electron beam.

通常の手段によつては電圧測定が困難な試料、
例えば微細なパターンを有する集積回路表面の所
望の領域の電圧を測定する電圧測定装置として、
その試料に電子ビームを照射してこれによつて発
生する二次電子の量を検出し、この二次電子量の
変化を試料の電位の変化と看做すことを基本原理
とする電圧測定装置がある。
Samples whose voltage is difficult to measure by conventional means,
For example, as a voltage measuring device that measures the voltage of a desired area on the surface of an integrated circuit having a fine pattern.
A voltage measurement device whose basic principle is to irradiate the sample with an electron beam, detect the amount of secondary electrons generated by this, and regard the change in the amount of secondary electrons as a change in the potential of the sample. There is.

この種の電圧測定装置の一例の基本的構成を第
1図に示す。図において、1は装置の外箱である
真空容器であり、2は電子ビーム3を試料4に照
射する電子銃であり、二次電子5を発生する。6
は引き出し電極であり、試料4よりも正電位にあ
る。又、7は分析用減速電極であり、二次電子量
検出器8に入射する二次電子量を制御する機能を
有する。
The basic configuration of an example of this type of voltage measuring device is shown in FIG. In the figure, 1 is a vacuum container that is the outer box of the apparatus, and 2 is an electron gun that irradiates a sample 4 with an electron beam 3 and generates secondary electrons 5. 6
is an extraction electrode and is at a more positive potential than sample 4. Further, 7 is a deceleration electrode for analysis, which has a function of controlling the amount of secondary electrons incident on the secondary electron amount detector 8.

かゝる構成を有する電圧測定装置における二次
電子量のその二次電子が有するエネルギーに対す
る分布は第2図aに示す如くであり、この分布曲
線は試料の電位をパラメータとしてX軸すなわち
エネルギー軸に沿つて平行移動するものと考えら
れている。図において、曲線A,Bは、夫々、試
料電圧が例えば5V、0Vの場合である。二次電子
量検出器に入射する二次電子量はエネルギーがあ
る一定値以上の二次電子の総量であり、又、二次
電子量検出器に入射する二次電子量は分析用減速
電圧によつて制御されるから、第2図aは、第2
図bの如く変換されうる。図において、曲線A′,
B′は夫々曲線A,Bに対応して試料電圧が例え
ば5V、0Vの場合である。
The distribution of the amount of secondary electrons with respect to the energy possessed by the secondary electrons in a voltage measuring device having such a configuration is as shown in Figure 2a, and this distribution curve is plotted along the X axis, that is, the energy axis, with the potential of the sample as a parameter. It is thought that the object moves in parallel along the . In the figure, curves A and B are for the case where the sample voltage is, for example, 5V and 0V, respectively. The amount of secondary electrons incident on the secondary electron amount detector is the total amount of secondary electrons with energy above a certain value, and the amount of secondary electrons incident on the secondary electron amount detector is the deceleration voltage for analysis. Therefore, Fig. 2a is controlled by
It can be converted as shown in Figure b. In the figure, curve A′,
B' corresponds to curves A and B, respectively, when the sample voltages are, for example, 5V and 0V.

そこで、試料の電位と減速電極の電圧以外の要
素であつて二次電子量に影響を及ばしうる要素は
すべて一定に保ち、減速電極の電圧のみをパラメ
ータとして変化させて、電位を異にする複数の試
料に対し、二次電子量検出器出力を一定にする減
速電圧を求めれば、減速電圧の差△V(第2図b
参照)をもつて試料相互間の電位差を求めること
ができる筈である。
Therefore, all the elements other than the potential of the sample and the voltage of the deceleration electrode that can affect the amount of secondary electrons are kept constant, and only the voltage of the deceleration electrode is changed as a parameter to change the potential. If the deceleration voltage that keeps the output of the secondary electron amount detector constant is determined for multiple samples, the difference in deceleration voltage △V (Fig. 2b
), it should be possible to determine the potential difference between the samples.

ところが、実験の結果によれば、二次電子量検
出器出力対分析用減速電極の電圧すなわち減速電
圧の関係を表わす曲線は第2図bに示す如くなら
ず往々、第3図に示す如くなる。すなわち、何ら
かの原因により、二次電子量検出器出力対減速電
圧の函数形態が減速電圧の変化とともに不整的に
変化する。図において、曲線A″,B″は夫々曲線
A′,B′に対応しており試料電圧が例えば5V、0V
の場合である。換言すれば、減速電圧を変化する
と、上記の函数形態が不整的に変化してしまう。
この傾向は、上記構成を有する電圧測定装置の測
定精度を著しく低下させるものである。
However, according to the results of experiments, the curve representing the relationship between the output of the secondary electron quantity detector and the voltage of the deceleration electrode for analysis, that is, the deceleration voltage, is not as shown in Fig. 2b, but often as shown in Fig. 3. . That is, for some reason, the function form of the output of the secondary electron amount detector versus the deceleration voltage changes irregularly as the deceleration voltage changes. In the figure, curves A″ and B″ are respectively curves.
Corresponds to A′ and B′, and the sample voltage is e.g. 5V, 0V.
This is the case. In other words, when the deceleration voltage is changed, the above function form changes irregularly.
This tendency significantly reduces the measurement accuracy of the voltage measuring device having the above configuration.

本発明は、この問題を解決することにあり、二
次電子量検出器出力対分析用減速電圧の函数形態
が減速電圧に追従して変化することのない特性を
有する、電子ビームによる電圧測定装置を提供す
ることにある。その要旨は、引き出し電極と分析
用減速電極との間を、これら電極と相似形を有す
るバツフアー電極をこれら電極と同心的に配置す
ることにある。
The present invention is aimed at solving this problem, and is a voltage measuring device using an electron beam, which has a characteristic that the function form of the output of a secondary electron quantity detector versus the analytical deceleration voltage does not change following the deceleration voltage. Our goal is to provide the following. The gist thereof is to arrange a buffer electrode having a similar shape to the extraction electrode and the deceleration electrode for analysis concentrically with these electrodes.

以下、図面を参照しつゝ、本発明の一実施例に
係る、電子ビームによる電圧測定装置について説
明し、本発明の構成と特有の効果とを明らかにす
る。
DESCRIPTION OF THE PREFERRED EMBODIMENTS A voltage measuring device using an electron beam according to an embodiment of the present invention will be described below with reference to the drawings, and the configuration and unique effects of the present invention will be clarified.

まず、上記の函数形態の不整的変化の理由につ
いて種々検討した結果、ある割合の二次電子が、
減速電極を通過するとき、減速電極に垂直でない
方向に飛行し、そのため、限界条件に近いエネル
ギーを有する二次電子のうちのある割合が検出器
に到達しないためであろうと推定される。更に、
かゝる二次電子飛行方向の異常は引き出し電極と
減速電極との間の電界の方向が影響しているもの
と推定される。すなわち、引き出し電極には通常
+1KV程度を印加して、二次電子を吸引するが、
分析用減速電極には通常−10〜0V程度を印加し
て二次電子速度を制御する。その結果、二次電子
の速度はこの区間において急速に減少することに
なり、いずれの電極も網状である等の影響があつ
て、両電極間の電界の方向が電極間に対し垂直で
はなくなり、飛行方向が電極面に対し垂直でない
二次電子が発生し、上記の函数形態の不整的変化
を招来するものと推定される。
First, as a result of various studies on the reasons for the irregular change in the function form mentioned above, we found that a certain proportion of secondary electrons
It is assumed that this is because when passing through the deceleration electrode, some fraction of the secondary electrons that fly in a direction that is not perpendicular to the deceleration electrode and therefore have energy close to the limit condition do not reach the detector. Furthermore,
It is presumed that this abnormality in the flight direction of the secondary electrons is affected by the direction of the electric field between the extraction electrode and the deceleration electrode. In other words, normally around +1KV is applied to the extraction electrode to attract secondary electrons, but
The speed of secondary electrons is usually controlled by applying a voltage of about -10 to 0 V to the deceleration electrode for analysis. As a result, the velocity of the secondary electrons rapidly decreases in this section, and because both electrodes are mesh-like, the direction of the electric field between the two electrodes is no longer perpendicular to the gap between the electrodes. It is presumed that secondary electrons whose flight direction is not perpendicular to the electrode surface are generated, causing the above-mentioned asymmetrical change in the function form.

この推定にもとづき、上記の欠点を解消するた
めには、引き出し電極と減速電極との間に第3の
電極(バツフアー電極)を設け、これに数10〜数
100V程度の正電圧を印加しておくことが有効で
あると考え、第4図に示す構造を有する電子ビー
ムによる電圧測定装置を試作し、実験を繰り返し
たところ、バツフアー電極に印加する電圧が50V
〜100V程度において、おゝむね良好な結果が得
られることが確認された。図において、1〜8は
夫々第1図に同一番号をもつて示すものと同一で
あり、9が本発明の構成要素であるバツフアー電
極であり、引き出し電極、減速電極と相似形の半
球形網状の形状を有し、両電極と同心的に配置さ
れている。
Based on this estimation, in order to eliminate the above drawback, a third electrode (buffer electrode) is provided between the extraction electrode and the deceleration electrode, and this
Thinking that it would be effective to apply a positive voltage of about 100V, we prototyped a voltage measurement device using an electron beam with the structure shown in Figure 4, and after repeated experiments, we found that the voltage applied to the buffer electrode was 50V.
It was confirmed that generally good results were obtained at about ~100V. In the figure, 1 to 8 are the same as those shown with the same numbers in FIG. It has the shape of , and is arranged concentrically with both electrodes.

以上、説明せるとおり、本発明によれば、
夫々、半径を異にする半球形網状の形状を有し同
心的に配置された引き出し電極と分析用減速電極
とを有し、二次電子量を検出してなす、電子ビー
ムによる電圧測定装置において、両電極の間に、
両電極と同心的に配置された半球形網状のバツフ
アー電極が設けてあるので、エネルギー分解能が
向上し、減速電圧の変化の影響を受けず、分析特
性の向上した、電子ビームによる電圧測定装置を
提供することができる。
As explained above, according to the present invention,
In a voltage measuring device using an electron beam, which has an extraction electrode and an analysis deceleration electrode, each having a hemispherical mesh shape with a different radius and arranged concentrically, and which detects the amount of secondary electrons. , between both electrodes,
A hemispherical net-like buffer electrode is placed concentrically with both electrodes, which improves energy resolution, is unaffected by changes in the deceleration voltage, and improves analytical characteristics of the electron beam voltage measuring device. can be provided.

尚、バツフアー電極に印加すべき電圧は減速電
圧との関係で決定される。
Note that the voltage to be applied to the buffer electrode is determined in relation to the deceleration voltage.

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

第1図は従来技術における、電子ビームによる
電圧測定装置の基本的構成を示す概念図であり、
第2図a,bは第1図に示す電子ビームによる電
圧測定装置の電圧測定原理を説明する補助グラフ
であり、第3図は従来技術における、電子ビーム
による電圧測定装置の欠点を説明する補助グラフ
であり、第4図は本発明の一実施例に係る、電子
ビームによる電圧測定装置の基本的構成を示す概
念図である。 1……外箱である真空容器、2……電子銃、3
……電子ビーム、4……試料、5……二次電子、
6……引き出し電極、7……分析用減速電極、8
……二次電子量検出装置、9……バツフアー電
極。
FIG. 1 is a conceptual diagram showing the basic configuration of a voltage measuring device using an electron beam in the prior art.
Figures 2a and b are supplementary graphs for explaining the voltage measurement principle of the voltage measuring device using an electron beam shown in Figure 1, and Figure 3 is a supplementary graph for explaining the drawbacks of the voltage measuring device using an electron beam in the prior art. FIG. 4 is a conceptual diagram showing the basic configuration of a voltage measuring device using an electron beam according to an embodiment of the present invention. 1... Vacuum container which is an outer box, 2... Electron gun, 3
...Electron beam, 4...Sample, 5...Secondary electron,
6...Extraction electrode, 7...Deceleration electrode for analysis, 8
...Secondary electron amount detection device, 9...Buffer electrode.

Claims (1)

【特許請求の範囲】[Claims] 1 夫々半径を異にする半球形網状の形状を有し
同心的に配置された引き出し電極と分析用減速電
極と、該半球形網状電極の中心に配置された試料
に電子ビームを照射する電子放出装置と、前記半
球形網状電極を通過した二次電子を検出する検出
装置とを有し、二次電子の有するエネルギーが電
子ビームの照射される試料の電位に依存する性質
を利用してなす電子ビームによる電圧測定装置に
おいて、前記引き出し電極と前記分析用減速電極
との間に、該電極と同心的に配置された半球形網
状のバツフアー電極を有することを特徴とする電
子ビームによる電圧測定装置。
1. An extraction electrode and an analytical deceleration electrode arranged concentrically, each having a hemispherical mesh shape with a different radius, and an electron emission device that irradiates the sample with an electron beam placed at the center of the hemispherical mesh electrode. and a detection device that detects the secondary electrons that have passed through the hemispherical mesh electrode, and the electron beam is generated by utilizing the property that the energy of the secondary electrons depends on the potential of the sample that is irradiated with the electron beam. A voltage measuring device using an electron beam, characterized in that the voltage measuring device using an electron beam has a hemispherical mesh buffer electrode arranged between the extraction electrode and the analysis deceleration electrode concentrically with the electrode.
JP56047106A 1981-03-30 1981-03-30 Voltage measuring device using electron beam Granted JPS57161556A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56047106A JPS57161556A (en) 1981-03-30 1981-03-30 Voltage measuring device using electron beam

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56047106A JPS57161556A (en) 1981-03-30 1981-03-30 Voltage measuring device using electron beam

Publications (2)

Publication Number Publication Date
JPS57161556A JPS57161556A (en) 1982-10-05
JPH0252828B2 true JPH0252828B2 (en) 1990-11-14

Family

ID=12765916

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56047106A Granted JPS57161556A (en) 1981-03-30 1981-03-30 Voltage measuring device using electron beam

Country Status (1)

Country Link
JP (1) JPS57161556A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2578744B2 (en) * 1984-09-03 1997-02-05 日本電気株式会社 Electronic beam measuring device

Also Published As

Publication number Publication date
JPS57161556A (en) 1982-10-05

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