JPS63205551A - Auger electron spectroscopic device - Google Patents

Auger electron spectroscopic device

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Publication number
JPS63205551A
JPS63205551A JP62037461A JP3746187A JPS63205551A JP S63205551 A JPS63205551 A JP S63205551A JP 62037461 A JP62037461 A JP 62037461A JP 3746187 A JP3746187 A JP 3746187A JP S63205551 A JPS63205551 A JP S63205551A
Authority
JP
Japan
Prior art keywords
signal
sample
detector
auger
auger 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.)
Pending
Application number
JP62037461A
Other languages
Japanese (ja)
Inventor
Satoru Sekine
哲 関根
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 JP62037461A priority Critical patent/JPS63205551A/en
Publication of JPS63205551A publication Critical patent/JPS63205551A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain a current Auger electron image by constituting a titled device in such a manner that an Auger electron detection signal is standardized by the signal detected by a reflected electron detector and said signal is introduced to a display device to observe the Auger electron image of a sample. CONSTITUTION:A scanning signal generator 9 supplies two-dimensional scanning signals to deflectors 8x, 8y and supplies the synchronized signals to deflectors 11x, 11y of a display device 10 as well. The reflected electron detector 12 is disposed between an incident slit 5a of a cylindrical mirror analyzer 3a and the sample 2. The detection signal of the detector 12 is supplied as a signal Sb via an amplifier 13 to a divider 14. On the other hand, the signal Sb of an Auger electron detector 6 is supplied to a divider 14 as well by which a signal ratio Sa/Sb is determined. The signals determined in such a manner are supplied as signals for modulating luminance of a device 10. The signal which is canceled in a surface shape effect is obtd. when the signal Sa is divided by Sb. The signal standardized by the signal of the reflected electrons is introduced as a luminance signal to the device 10, by which the correct Auger electron image is obtd.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はオージェ電子分光装置の改良、特に特定のエネ
ルギーを有するオージェ電子による試料画像を得る場合
や、特定エネルギーのオージェ電子によるラインスペク
トルを得る際に試料表面の凹凸の影響をなくしたオージ
ェ電子分光装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention is for improving Auger electron spectrometers, particularly for obtaining sample images using Auger electrons having a specific energy, and for obtaining line spectra using Auger electrons having a specific energy. This invention relates to an Auger electron spectrometer that eliminates the effects of unevenness on the surface of a sample.

[従来技術] オージェ電子分光法は、試料に集束電子線を照射したと
き、その試料から背面散乱する電子のエネルギーをエネ
ルギーアナライプを用いて分光し、試料の定性・定量分
析を行なうものであるが、オージェ電子はそのエネルギ
ーが低いので、試料の極表層部からしか発生しないので
、オージェ電子分光法は試料の表面分析技法として近時
脚光を浴び、急速に普及している。
[Prior art] Auger electron spectroscopy uses an energy analyzer to analyze the energy of electrons backscattered from a sample when the sample is irradiated with a focused electron beam, thereby performing qualitative and quantitative analysis of the sample. However, since Auger electrons have low energy and are only generated from the extreme surface layer of a sample, Auger electron spectroscopy has recently been in the spotlight as a technique for analyzing the surface of samples, and is rapidly becoming popular.

第3図は従来の一般的なオージェ電子分光装置の主要部
を示す概略図で、1は集束レンズであり、電子銃(図示
せず)からの電子線を細く集束し、試料2上に照射する
。3ば同軸的に円筒(又は半円筒)3a、3bを配置し
て構成したシリンドリカル・ミラー・アナライザで、内
n3aはアース電位に、外筒3bは可変の直流?!m4
から負の電圧−Voが印加されている。前記内筒3aに
はオージェ電子の入射用の環状スリット5aと出射用ス
リット5bがあり、試料2から発生したオージェ電子は
5aを通して内筒3aと外筒3bの間に入り、その中に
形成された分析電界によりエネルギー分析され、特定の
エネルギーを有する電子が出射用スリット5bから取出
され、検出器6に入射する。この検出器の出力信号は増
幅器7により増幅され、適宜信号処理された後、陰極線
管等の表示装置又は記録装置に導入される。8x、8V
は電子線の偏向器であり、試料上で電子線を所望に走査
しあるいは移動させるためのものである。
Figure 3 is a schematic diagram showing the main parts of a conventional general Auger electron spectrometer. 1 is a focusing lens, which narrowly focuses the electron beam from an electron gun (not shown) and irradiates it onto the sample 2. do. 3 is a cylindrical mirror analyzer configured by coaxially arranging cylinders (or semi-cylinders) 3a and 3b, the inner cylinder 3a is at ground potential, and the outer cylinder 3b is a variable DC? ! m4
A negative voltage -Vo is applied from. The inner cylinder 3a has an annular slit 5a for the incidence of Auger electrons and an annular slit 5b for output, and the Auger electrons generated from the sample 2 enter between the inner cylinder 3a and the outer cylinder 3b through 5a and are formed therein. The energy of the electrons is analyzed by the analysis electric field, and electrons having a specific energy are extracted from the emission slit 5b and enter the detector 6. The output signal of this detector is amplified by an amplifier 7, subjected to appropriate signal processing, and then introduced to a display device such as a cathode ray tube or a recording device. 8x, 8V
is an electron beam deflector, and is used to scan or move the electron beam on the sample as desired.

前記陰極線管等の表示装置はこの電−子線偏向器と同期
しており、検出信号を輝度信号として陰極線管に導入す
ると該陰極線管上には試料のオージェ電子像が形成され
る。又、外筒3bに印加する電圧Voを変化させると出
射用スリット5bから出射するオージェ電子のエネルギ
ーが変化するので、該電圧を一定範囲にわたり掃引する
ことによりオージェ電子のラインスペクトルが得られる
A display device such as the cathode ray tube is synchronized with this electron beam deflector, and when a detection signal is introduced into the cathode ray tube as a luminance signal, an Auger electron image of the sample is formed on the cathode ray tube. Furthermore, since the energy of Auger electrons emitted from the emission slit 5b changes when the voltage Vo applied to the outer tube 3b is changed, a line spectrum of Auger electrons can be obtained by sweeping the voltage over a certain range.

[発明が解決しようとする問題点] ところが、第4図に示すように試料2の表面に凹凸があ
る場合には、水平面■に対してシリンドリカル・ミラー
・アナライザ側に傾斜した面■では、第5図に示すよう
にスペクトル強度は強くなり、又逆にアナライザと反対
側に傾斜した面■ではスペクトル強度は小さくなる。第
5図において、縦軸は検出強度、横軸はオージェ電子の
エネルギーである。従って、従来の装置でオージェ電子
像(元素分布像)を得ようとしても、表面に凹凸を有す
る試料では表面形状の影響のため、正しい組成像が得ら
れなかった。
[Problems to be Solved by the Invention] However, when the surface of the sample 2 is uneven as shown in FIG. As shown in FIG. 5, the spectral intensity becomes strong, and conversely, the spectral intensity becomes small on the surface (2) inclined toward the side opposite to the analyzer. In FIG. 5, the vertical axis represents the detected intensity, and the horizontal axis represents the energy of Auger electrons. Therefore, even if an attempt was made to obtain an Auger electron image (element distribution image) using a conventional apparatus, a correct compositional image could not be obtained with a sample having an uneven surface due to the influence of the surface shape.

本発明は上記点に鑑み、試料の表面状態に関係なく正確
な組成像を得ることの可能なオージェ電子分光装置を提
供することに目的がある。
In view of the above-mentioned points, an object of the present invention is to provide an Auger electron spectrometer capable of obtaining an accurate compositional image regardless of the surface condition of a sample.

[問題を解決するための手段] 本発明は集束電子線を試料上に照射する手段、該電子線
を試料上で任意に走査移動するための偏向系、前記電子
線の照射により試料から発生ずるオージェ電子のエネル
ギーを分光するためのエネルギーアナライプ、このエネ
ルギーアナライザで分光されたオージェ電子を検出する
検出器及びその検出信号が導入される表示装置又は記録
装置を有した装置において、前記エネルギーアナライザ
の前方に反射電子の検出器を配置し、前記エネルギーア
ナライザで分光され、検出器で検出されたオージェ電子
信号Saと前記反射電子°の検出信号Sbとの比S a
/S bを求める手段を備え、該信号Sa/Sbを前記
表示装置や記録装置に導入したオージェ電子分光装置に
特徴がある。
[Means for Solving the Problem] The present invention provides a means for irradiating a sample with a focused electron beam, a deflection system for arbitrarily scanning and moving the electron beam on the sample, and a means for irradiating a focused electron beam onto a sample. An apparatus comprising an energy analyzer for dispersing the energy of Auger electrons, a detector for detecting the Auger electrons separated by the energy analyzer, and a display device or a recording device into which the detection signal is introduced. A backscattered electron detector is placed in front, and the ratio S a of the Auger electron signal Sa, which is spectrally spectrally analyzed by the energy analyzer and detected by the detector, and the detection signal Sb of the backscattered electrons.
The Auger electron spectroscopy apparatus is characterized in that it is equipped with a means for determining Sa/Sb and introduces the signal Sa/Sb into the display device or recording device.

[作用] 本発明においては、オージェ電子の検出器の他にエネル
ギーアナライザの前方に反射電子の検出器を置き、オー
ジェ電子の検出信号と反IJ4i!!子の検出信号の比
を求め、類比の信号を表示装置に導入し、エネルギーア
ナライザに入射するオージェ電子の試料表面による影響
を除去するようにしている。
[Function] In the present invention, in addition to the Auger electron detector, a backscattered electron detector is placed in front of the energy analyzer, and the Auger electron detection signal and the anti-IJ4i! ! The ratio of the analogous detection signals is calculated, and the analogous signal is introduced into the display device to eliminate the influence of the sample surface on Auger electrons incident on the energy analyzer.

[実施例] 第1図は本発明の一実施例を示ずブロック線図であり、
第3図と同符号は同様な構成要素を示しである。同図に
おいて、9は走査信号発生器であり、前記電子線の偏向
器Qx、ayに2次元的な走査信号を供給すると共に、
表示装置10の偏向器11X、11Vにも同期した信号
を供給している。シリンドリカル・ミラー・アナライザ
の内筒3aの入射スリット5aと試料2の間(エネルギ
ーアナライザの前方)には試料2に電子線を照射した際
、該試料表面から反射する電子を検出する検出器12が
配置されている。この検出器としては例えば小形に形成
できる半導体検出器(P−N接合検出器)が使用され、
その検出信号は増幅器13を介して信号sbとして割算
器14に供給される。前記オージェ電子検出器の信号S
aも割算器14に供給され、前記反射電子の検出信号S
bとの比Sa/Sbが求められる。このようにして求め
られた信号は表示装置10の輝度変調信号として供給さ
れ。表示装置上に特定エネルギー(特定元素)の像を形
成する。
[Embodiment] FIG. 1 is a block diagram showing an embodiment of the present invention.
The same reference numerals as in FIG. 3 indicate similar components. In the figure, 9 is a scanning signal generator that supplies two-dimensional scanning signals to the electron beam deflectors Qx and ay, and
A synchronized signal is also supplied to the deflectors 11X and 11V of the display device 10. Between the entrance slit 5a of the inner cylinder 3a of the cylindrical mirror analyzer and the sample 2 (in front of the energy analyzer), there is a detector 12 that detects electrons reflected from the sample surface when the sample 2 is irradiated with an electron beam. It is located. As this detector, for example, a semiconductor detector (P-N junction detector) that can be formed into a small size is used.
The detection signal is supplied to a divider 14 via an amplifier 13 as a signal sb. Signal S of the Auger electron detector
a is also supplied to the divider 14, and the reflected electron detection signal S
The ratio Sa/Sb with b is determined. The signal obtained in this manner is supplied as a brightness modulation signal to the display device 10. An image of a specific energy (specific element) is formed on a display device.

このような装置において、検出器12で検出される反t
JJ電子の信号sbは、該検出器がオージェ電子の検出
方向(エネルギーアナライザの前方)に置かれているの
で、オージェ電子の検出信号Saと同様な試料表面形状
効果を受けており、従ってオージェ電子の信号Saを反
射電子の信号sbで割算すると表面形状効果がキャンセ
ルされた信号になる。この反射電子の信号により規格化
された信号を表示装置に輝度信号として導入することに
より、表面形状の影響のほとんどないオージェ電子像を
得ることができる。
In such a device, the anti-t detected by the detector 12
Since the JJ electron signal sb is placed in the Auger electron detection direction (in front of the energy analyzer), the JJ electron signal sb is subject to the same sample surface shape effect as the Auger electron detection signal Sa. Dividing the signal Sa by the signal sb of the reflected electrons results in a signal in which the surface shape effect is canceled. By introducing a signal normalized by the reflected electron signal into a display device as a luminance signal, an Auger electron image almost unaffected by the surface shape can be obtained.

第2図は本発明の他の実施例の主要部であり、オージェ
電子検出器の増幅器7及び反射電子の検出器13として
対数増幅器を使用し9、夫々log。
FIG. 2 shows the main part of another embodiment of the present invention, in which logarithmic amplifiers are used as the amplifier 7 of the Auger electron detector and the backscattered electron detector 13, respectively.

Sa及びlog、9bの信号を得、引算回路15でその
引算(I oa、Sa−l、oQ、Sb)を行ない、そ
の結果を真数増幅器16により真数に変換し、Sa/S
bの信号を得るように構成したもので、第1図の割粋器
と全く同様な結果が得られる。
The signals Sa, log, and 9b are obtained, and the subtraction circuit 15 performs subtraction (I oa, Sa-l, oQ, Sb), and the result is converted into an antilog by the antilog amplifier 16, and Sa/S
This is configured to obtain the signal b, and the result is exactly the same as that of the divider shown in FIG.

[効果1 以上説明したように、本発明ではオージェ電子エネルギ
ーアナライザの入射口に反射電子検出器を設置し、この
検出器で検出された信号によりオージェ電子検出信号を
規格化し、その信号を表示装置に導入して試料のオージ
ェ電子懺を観察するように構成しているので、試料の表
面に凹凸が存在しても、その凹凸は全てキャンセルされ
、試料表面の形状効果のほとんどない正しいオージェ電
子像を得ることができる。
[Effect 1 As explained above, in the present invention, a backscattered electron detector is installed at the entrance of the Auger electron energy analyzer, the Auger electron detection signal is normalized by the signal detected by this detector, and the signal is displayed on the display device. Since the structure is such that the Auger electron beam of the sample is observed by introducing the sample into 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を示すプOツ、りI!図、第
2図は本発明の他の実施例を示す主要部のブロック線図
、第3図は従来のオージェ電子分光装置の主要部を示す
図、第4図及び第5図は第3図の欠点を説明する図であ
る。 1:集束レンズ    2:試料 3ニジリントリカル・ミラー・アナライザ3a:内筒 
     3b:外筒 4:直流電It!      5a:入射スリット5b
=出射スリツト 6:オージェ電子検出器 7:増幅器      Bx、sy:偏向器9:走査信
号発生器 10:表示装置 11X、11V:表示装置の偏向器 12:反射電子検出器 13:増幅器 14:割算器     15:引算器 16二真数増幅器
FIG. 1 shows an embodiment of the present invention. 2 is a block diagram of the main parts showing another embodiment of the present invention, FIG. 3 is a diagram showing the main parts of a conventional Auger electron spectrometer, and FIGS. FIG. 1: Focusing lens 2: Sample 3 Nijilintrical mirror analyzer 3a: Inner cylinder
3b: Outer cylinder 4: DC electric It! 5a: entrance slit 5b
= Output slit 6: Auger electron detector 7: Amplifier Bx, sy: Deflector 9: Scanning signal generator 10: Display device 11X, 11V: Display device deflector 12: Backscattered electron detector 13: Amplifier 14: Division Device 15: Subtractor 16 Two-log amplifier

Claims (1)

【特許請求の範囲】[Claims] 集束電子線を試料上に照射する手段、該電子線を試料上
で任意に走査移動するための偏向系、前記電子線の照射
により試料から発生するオージェ電子のエネルギーを分
光するためのエネルギーアナライザ、このエネルギーア
ナライザで分光されたオージェ電子を検出する検出器及
びその検出信号が導入される表示装置又は記録装置を有
した装置において、前記エネルギーアナライザの前方に
反射電子の検出器を配置し、前記エネルギーアナライザ
で分光され、検出器で検出されたオージェ電子信号Sa
と前記反射電子の検出信号Sbとの比Sa/Sbを求め
る手段を備え、この信号Sa/Sbを前記表示装置や記
録装置に導入するように構成したことを特徴とするオー
ジェ電子分光装置。
means for irradiating a sample with a focused electron beam; a deflection system for arbitrarily scanning and moving the electron beam on the sample; an energy analyzer for dispersing the energy of Auger electrons generated from the sample by irradiation with the electron beam; In this device, which has a detector for detecting Auger electrons spectrally spectrolated by the energy analyzer, and a display device or a recording device into which the detection signal is introduced, a backscattered electron detector is disposed in front of the energy analyzer, and Auger electron signal Sa spectrally analyzed by the analyzer and detected by the detector
and the detection signal Sb of the reflected electrons, the Auger electron spectrometer comprising means for determining the ratio Sa/Sb of the reflected electrons and the reflected electron detection signal Sb, and is configured to introduce the signal Sa/Sb into the display device or the recording device.
JP62037461A 1987-02-20 1987-02-20 Auger electron spectroscopic device Pending JPS63205551A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62037461A JPS63205551A (en) 1987-02-20 1987-02-20 Auger electron spectroscopic device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62037461A JPS63205551A (en) 1987-02-20 1987-02-20 Auger electron spectroscopic device

Publications (1)

Publication Number Publication Date
JPS63205551A true JPS63205551A (en) 1988-08-25

Family

ID=12498167

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62037461A Pending JPS63205551A (en) 1987-02-20 1987-02-20 Auger electron spectroscopic device

Country Status (1)

Country Link
JP (1) JPS63205551A (en)

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