JP2903874B2 - Ion-excitation X-ray analyzer with focused ion beam - Google Patents
Ion-excitation X-ray analyzer with focused ion beamInfo
- Publication number
- JP2903874B2 JP2903874B2 JP4172249A JP17224992A JP2903874B2 JP 2903874 B2 JP2903874 B2 JP 2903874B2 JP 4172249 A JP4172249 A JP 4172249A JP 17224992 A JP17224992 A JP 17224992A JP 2903874 B2 JP2903874 B2 JP 2903874B2
- Authority
- JP
- Japan
- Prior art keywords
- sample
- ray
- ion
- ion beam
- characteristic
- 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
Links
- 238000010884 ion-beam technique Methods 0.000 title claims description 13
- 238000010849 ion bombardment Methods 0.000 claims description 2
- 150000002500 ions Chemical group 0.000 description 9
- 238000002441 X-ray diffraction Methods 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 230000005284 excitation Effects 0.000 description 2
- 238000000605 extraction Methods 0.000 description 2
- 229910001338 liquidmetal Inorganic materials 0.000 description 2
- UZHDGDDPOPDJGM-UHFFFAOYSA-N Stigmatellin A Natural products COC1=CC(OC)=C2C(=O)C(C)=C(CCC(C)C(OC)C(C)C(C=CC=CC(C)=CC)OC)OC2=C1O UZHDGDDPOPDJGM-UHFFFAOYSA-N 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000010894 electron beam technology Methods 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 238000005211 surface analysis Methods 0.000 description 1
Landscapes
- Analysing Materials By The Use Of Radiation (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明はイオン励起型X線分析装
置に関し、さらに詳しくは表面から数原子層の組成に関
する情報を優先的に検出する表面分析装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an ion-excited X-ray analyzer, and more particularly to a surface analyzer for preferentially detecting information on the composition of several atomic layers from the surface.
【0002】[0002]
【従来の技術】細く絞ったイオンビームを試料上で走査
するイオンビーム照射系を持った測定手段としては従
来、二次イオン質量分析装置(SIMS),集束イオン
ビーム(FIB)が知られている。また照射系として電
子ビームを用いた場合、発生する特性X線を検出して表
面の組成を知る手段としては走査型電子顕微鏡(SE
M),X線マイクロアナライザ(XMA),透過型電子
顕微鏡(TEM)等が一般的に用いられている。ここで
は本発明にもっとも近いと考えられるFIBにX線半導
体検出器を配設した従来技術について特徴をのべる。F
IBの場合、イオンは30kV程度の加速電圧によって
加速され、試料表面に照射される。この場合イオンは表
面から数nmの深さまで浸入し、表面原子をスパッタす
ると同時に表面原子との相互作用によって二次電子、特
性X線等を発生させる。イオンの侵入深さが数nmであ
ることから二次励起による特性X線を無視すれば、FI
BによるX線分析はXMA等に比べればより表面の情報
を有していると考えられる。2. Description of the Related Art Conventionally, a secondary ion mass spectrometer (SIMS) and a focused ion beam (FIB) are known as a measuring means having an ion beam irradiation system for scanning a finely focused ion beam on a sample. . When an electron beam is used as the irradiation system, a scanning electron microscope (SE
M), an X-ray microanalyzer (XMA), a transmission electron microscope (TEM) and the like are generally used. Here, the features of the prior art in which an X-ray semiconductor detector is arranged in the FIB which is considered to be closest to the present invention will be described. F
In the case of IB, ions are accelerated by an accelerating voltage of about 30 kV and are irradiated on the sample surface. In this case, the ions penetrate to a depth of several nm from the surface and sputter the surface atoms, and at the same time, generate secondary electrons, characteristic X-rays, and the like by interaction with the surface atoms. Since the penetration depth of ions is several nm, if the characteristic X-rays due to secondary excitation are ignored, FI
It is considered that X-ray analysis using B has more surface information than XMA or the like.
【0003】[0003]
【発明が解決しようとする課題】FIBによるX線分析
は上述しように表面の組成に敏感な測定法ではあるが、
従来のFIBはX線検出器を試料表面に対して30°〜
50°と適当な位置に配置していたため、表面組成に敏
感な情報が充分に得られない。本発明は、従来よりもさ
らに表面の組成に敏感な情報が得られる装置を提供する
ことがねらいである。The X-ray analysis by FIB is a measurement method which is sensitive to the surface composition as described above.
The conventional FIB uses an X-ray detector at 30 ° to the sample surface.
Since it was arranged at an appropriate position of 50 °, sufficient information sensitive to the surface composition could not be obtained. An object of the present invention is to provide a device capable of obtaining information more sensitive to the composition of the surface than before.
【0004】[0004]
【課題を解決するための手段】本発明は、細く絞ったイ
オンビームを試料上で走査するイオンビーム照射系と、
イオン衝撃により試料表面から発生する特性X線を検出
するX線検出器を有するイオン励起型X線分析装置にお
いて、試料におけるX線の全反射臨界角の方向にX線検
出器を配設して成ることを特徴とする構成になってい
る。According to the present invention, there is provided an ion beam irradiation system for scanning a narrowly focused ion beam on a sample,
In an ion excitation type X-ray analyzer having an X-ray detector for detecting characteristic X-rays generated from a sample surface due to ion bombardment, an X-ray detector is arranged in a direction of a critical angle of total reflection of X-rays in the sample. It is a configuration characterized by the following.
【0005】[0005]
【作用】本発明の要旨とするところは、X線検出器を全
反射臨界角と同じ取り出し角を有する方向に置くことに
より、試料のごく表面で発生した特性X線のみを優先的
に検出することにある。The gist of the present invention is that, by placing an X-ray detector in a direction having the same extraction angle as the critical angle for total reflection, only the characteristic X-rays generated on the very surface of the sample are detected preferentially. It is in.
【0006】光学的に平坦な鏡面を有する基板に、その
基板の持つ全反射臨界角よりも低い角度でX線を入射さ
せると全反射現象が起こる。この全反射臨界角φcritは
次式で表される。When an X-ray is incident on a substrate having an optically flat mirror surface at an angle lower than the total reflection critical angle of the substrate, a total reflection phenomenon occurs. This critical angle for total reflection φ crit is expressed by the following equation.
【0007】φcrit≒1.64×10-5√(ρ)・λ ここでλは入射X線の波長、ρは基板の密度である。Φ crit ≒ 1.64 × 10 −5 √ (ρ) · λ where λ is the wavelength of the incident X-ray and ρ is the density of the substrate.
【0008】図3は入射イオンが表面から数nmの深さ
まで進入した場合の様子を示した説明図である。FIB
の場合、入射イオンビーム1は試料2の表面2aから数
nmの深さA1 まで進入する。試料内に進入したイオン
はA0 からA1 までの深さの原子を励起し、特性X線を
励起させる。特性X線はあらゆる方向に等方的に発生す
るが、そのうち試料表面に平行なA0 O方向に発生した
X線は光線逆行の原理によりO点で屈折して臨界角φ
critの方向OA0 ′に進む。表面より深い部分A1 で表
面に平行な方向A1 O′方向に発生した特性X線は試料
中を直進する。A1 から表面方向A1 O方向に発生した
特性X線はO点で屈折して臨界角φcritよりも大きい角
度φcrit+αの方向OA1 ′方向に進む。従って臨界角
φcrit方向に置いたX線検出器によって検出される特性
X線は表面でA0 O方向に発生した特性X線のみとな
る。試料からX線検出器までの距離(数cm)はイオン
ビームの照射範囲(数十μm)に比べて格段に大きく入
射点の移動によるX線検出器の取出し角の変動は無視で
きる。以上のようにこの方法によれば試料のごく表面に
存在する原子のみを高精度に分析することができる。FIG. 3 is an explanatory view showing a state in which incident ions have penetrated from the surface to a depth of several nm. FIB
Cases, the incident ion beam 1 enters to a depth A 1 of a few nm from the surface 2a of the sample 2. The ions that have entered the sample excite atoms at a depth from A 0 to A 1 and excite characteristic X-rays. Characteristic X-rays are generated isotropically in all directions. Among them, X-rays generated in the A 0 O direction parallel to the sample surface are refracted at point O by the principle of light beam regression, and the critical angle φ
Proceed in the direction OA 0 'of crit . Surface deeper portion A 1 characteristic X-rays generated in a direction parallel A 1 O 'direction to the surface in the straight through the sample. Characteristic X-rays generated from A 1 toward the surface A 1 O direction travels refracted at point O in the direction OA 1 'direction of the large angle phi crit + alpha than the critical angle phi crit. Therefore, the characteristic X-rays detected by the X-ray detector placed in the critical angle φ crit direction are only characteristic X-rays generated in the A 0 O direction on the surface. The distance (several cm) from the sample to the X-ray detector is much larger than the irradiation range (several tens μm) of the ion beam, and the change in the extraction angle of the X-ray detector due to the movement of the incident point can be ignored. As described above, according to this method, only atoms existing on the very surface of the sample can be analyzed with high accuracy.
【0009】[0009]
【実施例】以下、本発明の一実施例について図1を参照
して説明する。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described below with reference to FIG.
【0010】図2は本発明のFIBによるイオン励起型
X線分析装置の一実施例を示す概略構成図で、図1は要
部拡大図である。図において、本実施例は細く絞ったイ
オンビーム1を試料2の表面に照射し、像観察を行なう
FIB部3と、発生した特性X線4をスリット5を通し
て試料の全反射臨界角φcritと同じ取り出し角を有すよ
うに配設されたX線検出器6から構成される。FIG. 2 is a schematic diagram showing one embodiment of an ion-excited X-ray analyzer using FIB according to the present invention, and FIG. 1 is an enlarged view of a main part. In this figure, in this embodiment, a FIB unit 3 for irradiating a finely focused ion beam 1 onto the surface of a sample 2 and observing an image, and generating a characteristic X-ray 4 through a slit 5 to determine the total reflection critical angle φ crit of the sample. It comprises an X-ray detector 6 arranged so as to have the same take-out angle.
【0011】以上のようにしてX線分析を行なうことに
より、試料のごく表面に存在する原子のみを高精度に分
析することができた。By performing the X-ray analysis as described above, it was possible to analyze only the atoms existing on the very surface of the sample with high accuracy.
【0012】なお、FIB部3は、図2に示す如く、液
体金属イオン源7,エキストラクタ8,電流モニタ9,
コンデンサレズ10,ビームブランカ11,可動絞1
2、スティグメータ13,対物レンズ14,偏向電極1
5,2次電子検出器16,スリット5から成り、従来装
置と同じ構成であるので説明は省略する。As shown in FIG. 2, the FIB unit 3 includes a liquid metal ion source 7, an extractor 8, a current monitor 9,
Condenser lesbian 10, beam blanker 11, movable aperture 1
2. Stigmeter 13, objective lens 14, deflection electrode 1
5, the secondary electron detector 16 and the slit 5, which have the same configuration as that of the conventional device, and a description thereof will be omitted.
【0013】[0013]
【発明の効果】以上説明したように、本発明のFIBに
よるイオン励起型X線分析装置によれば、試料のごく表
面に存在する原子から発生した特性X線のみを検出する
ように検出器が配設されているので、試料の表面分析に
最適であり表面組成について正確な測定が可能となる。As described above, according to the ion-excited X-ray analyzer using the FIB of the present invention, the detector is designed to detect only characteristic X-rays generated from atoms existing on the very surface of the sample. Since it is provided, it is optimal for surface analysis of a sample, and enables accurate measurement of the surface composition.
【図1】本発明の一実施例の要部拡大図。FIG. 1 is an enlarged view of a main part of an embodiment of the present invention.
【図2】本発明の一実施例の概略構成図。FIG. 2 is a schematic configuration diagram of one embodiment of the present invention.
【図3】本装置の原理を示す説明図。FIG. 3 is an explanatory view showing the principle of the present apparatus.
1 イオンビーム 2 試料表面 3 FIB部 4 特性X線 5 スリット 6 X線検出器 7 液体金属イオン源 8 エキストラクタ 9 電流モニタ 10 コンデンサレンズ 11 ビームブランカ 12 可動絞 13 スティグメータ 14 対物レンズ 15 偏向電極 16 2次電子検出器 DESCRIPTION OF SYMBOLS 1 Ion beam 2 Sample surface 3 FIB part 4 Characteristic X-ray 5 Slit 6 X-ray detector 7 Liquid metal ion source 8 Extractor 9 Current monitor 10 Condenser lens 11 Beam blanker 12 Movable aperture 13 Stig meter 14 Objective lens 15 Deflection electrode 16 Secondary electron detector
Claims (1)
するイオンビーム照射系と、イオン衝撃により試料表面
から発生する特性X線を検出するX線検出器を有し、か
つ試料におけるX線の全反射臨界角の方向に前記X線検
出器を配設して成ることを特徴とする集束イオンビーム
によるイオン励起型X線分析装置。1. An ion beam irradiation system for scanning a narrowly focused ion beam on a sample, an X-ray detector for detecting characteristic X-rays generated from the surface of the sample by ion bombardment, and detecting an X-ray on the sample. An ion-excited X-ray analyzer using a focused ion beam, wherein the X-ray detector is arranged in a direction of a critical angle of total reflection.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4172249A JP2903874B2 (en) | 1992-06-30 | 1992-06-30 | Ion-excitation X-ray analyzer with focused ion beam |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4172249A JP2903874B2 (en) | 1992-06-30 | 1992-06-30 | Ion-excitation X-ray analyzer with focused ion beam |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0613012A JPH0613012A (en) | 1994-01-21 |
JP2903874B2 true JP2903874B2 (en) | 1999-06-14 |
Family
ID=15938391
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4172249A Expired - Lifetime JP2903874B2 (en) | 1992-06-30 | 1992-06-30 | Ion-excitation X-ray analyzer with focused ion beam |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2903874B2 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP4665143B2 (en) * | 2005-03-18 | 2011-04-06 | 独立行政法人物質・材料研究機構 | Elemental analysis / evaluation method and apparatus in conductor samples by low energy ion irradiation |
JP4735805B2 (en) * | 2005-03-18 | 2011-07-27 | 独立行政法人物質・材料研究機構 | Method and apparatus for generating characteristic X-rays from conductive materials by low energy ion irradiation |
-
1992
- 1992-06-30 JP JP4172249A patent/JP2903874B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPH0613012A (en) | 1994-01-21 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
A01 | Written decision to grant a patent or to grant a registration (utility model) |
Free format text: JAPANESE INTERMEDIATE CODE: A01 Effective date: 19990223 |