JP2901637B2 - Scanning X-ray microscope - Google Patents
Scanning X-ray microscopeInfo
- Publication number
- JP2901637B2 JP2901637B2 JP8790789A JP8790789A JP2901637B2 JP 2901637 B2 JP2901637 B2 JP 2901637B2 JP 8790789 A JP8790789 A JP 8790789A JP 8790789 A JP8790789 A JP 8790789A JP 2901637 B2 JP2901637 B2 JP 2901637B2
- Authority
- JP
- Japan
- Prior art keywords
- ray
- scanning
- sample
- rays
- fluorescent
- 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
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- Analysing Materials By The Use Of Radiation (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は蛍光(あるいは散乱)X線を画像信号として
利用する走査型X線顕微鏡において、そのコントラスト
生成方法、特に試料表面の凹凸形状に対応した陰影コン
トラストを生成する走査型X線顕微鏡に関する。The present invention relates to a scanning X-ray microscope using fluorescent (or scattered) X-rays as an image signal, and a method for producing a contrast thereof, and particularly, to a method of forming irregularities on a sample surface. The present invention relates to a scanning X-ray microscope for generating a shadow contrast.
従来、蛍光X線を検出する形式の走査型X線顕微鏡
が、ジヤパニーズ,ジヤーナル,オブ、アプライド、フ
イジツクス第26巻(1987年)第L1260頁からL1262頁(Jp
n.J.Appl.phys.26(1987)ppL1260−1262)において報
告されている。Conventionally, a scanning X-ray microscope for detecting fluorescent X-rays has been disclosed in Japanese, Journal, Ob, Applied, Physics, Vol. 26 (1987), pages L1260 to L1262 (Jp.
nJAppl.phys. 26 (1987) ppL1260-1262).
この場合の信号強度は試料の各点での蛍光X線のエネ
ルギーによつて識別される特定元素の存在量(あるいは
濃度)に相当する。したがつて上記文献の装置によつて
元素毎のマツピングに相当する走査X線顕微鏡画像が得
られる。The signal intensity in this case corresponds to the abundance (or concentration) of the specific element identified by the energy of the fluorescent X-ray at each point of the sample. Accordingly, a scanning X-ray microscope image corresponding to the mapping for each element can be obtained by the apparatus described in the above document.
しかしながら、上記従来技術ではX線の入射方向及び
蛍光X線の観測方向に対する信号強度の依存性について
考慮されていない。このため、走査型電子顕微鏡のよう
な試料表面の形状にもとづく凹凸コントラストは観測さ
れていない。However, the above prior art does not consider the dependence of signal intensity on the incident direction of X-rays and the observation direction of fluorescent X-rays. For this reason, no concavo-convex contrast based on the shape of the sample surface as in a scanning electron microscope is observed.
本発明は、走査型X線顕微鏡において、試料表面の凹
凸による検出信号コントラストを生成し、あたかも可視
光を斜に入射させて試料を観察したような立体的な陰影
を有する画像を表示させることを目的としてなされたも
のである。The present invention provides a scanning X-ray microscope that generates a detection signal contrast due to irregularities on the surface of a sample and displays an image having a three-dimensional shadow as if observing the sample by obliquely incident visible light. It was made for the purpose.
上記目的を達成するために、本発明においては、試料
に照射させるX線の入射方向を試料表面にほぼ直角にす
ると共に、蛍光(あるいは散乱)X線検出方向を試料表
面に対して浅い角度内に限定すると共に、さらにその36
0に分布する試料表面に対する浅い放出角を有する成分
中の特定の放出方向の信号のみを画像信号として利用し
たものである。In order to achieve the above object, according to the present invention, the incident direction of the X-ray irradiating the sample is made substantially perpendicular to the sample surface, and the fluorescent (or scattered) X-ray detection direction is set at a shallow angle with respect to the sample surface. And 36
Only a signal in a specific emission direction in a component having a shallow emission angle with respect to the sample surface distributed to 0 is used as an image signal.
本発明の作用を第1図に従つて説明する。 The operation of the present invention will be described with reference to FIG.
単純化するために平坦な試料表面上に1個の凸部があ
る場合について述べる。試料上のAの位置が入射X線ビ
ームで照射される場合は、蛍光(あるいは散乱)X線は
検出器に到達する。しかしながら、試料を走査して、入
射X線がBの位置に入射するようにした場合は放出X線
が検出器に対して試料上の凸部でさえぎられ、吸収され
るために検出される蛍光(あるいは散乱)X線強度は点
Aの場合と比べて弱くなる。したがつて走査X線顕微鏡
像としては点Aは明るく点Bは暗く表示される。それに
よつて、あたかも可視光を試料面に斜に照射して直上か
ら写真を撮つた場合のように、試料表面の凹凸が陰影の
コントラストとして観察出来る。For the sake of simplicity, a case where there is one projection on a flat sample surface will be described. When the position A on the sample is irradiated with the incident X-ray beam, the fluorescent (or scattered) X-rays reach the detector. However, when the sample is scanned so that the incident X-rays are incident on the position B, the emitted X-rays are intercepted by the convex portion on the sample with respect to the detector and are detected because they are absorbed. The (or scattering) X-ray intensity is weaker than at point A. Therefore, point A is displayed bright and point B is displayed dark as a scanning X-ray microscope image. As a result, the unevenness of the sample surface can be observed as a shadow contrast, as if a visible light was obliquely applied to the sample surface and a photograph was taken from directly above.
以下、本発明の一実施例を第2図により説明する。X
線発生装置5から放射されるX線をX線集光鏡6を用い
てマイクロX線ビーム3として試料1上に入射させる。
試料1は試料走査機構7によつて二次元走査される。試
料1より放出される蛍光X線4はX線検出器2によつて
計数される。検出したX線信号は計測画像処理用計算機
8に送られる。また計算機8は試料走査機構5を制御し
ている。Hereinafter, an embodiment of the present invention will be described with reference to FIG. X
X-rays emitted from the ray generator 5 are incident on the sample 1 as micro X-ray beams 3 using the X-ray focusing mirror 6.
The sample 1 is two-dimensionally scanned by the sample scanning mechanism 7. The fluorescent X-rays 4 emitted from the sample 1 are counted by the X-ray detector 2. The detected X-ray signal is sent to the measurement image processing computer 8. The computer 8 controls the sample scanning mechanism 5.
二次元の走査X線顕微鏡像を計測するためには試料1
を二次元に走査すると同時に各点における蛍光X線強度
を計数し、その情報を計算機8のメモリに保存してお
く。デイスプレイ9に試料1上の各点における蛍光X線
強度に対応した画面の輝度を与えることによつて画像が
表示される。In order to measure a two-dimensional scanning X-ray microscope image, sample 1
Is scanned two-dimensionally and the fluorescent X-ray intensity at each point is counted, and the information is stored in the memory of the computer 8. An image is displayed by giving the display 9 a screen brightness corresponding to the fluorescent X-ray intensity at each point on the sample 1.
本発明によれば、蛍光(あるいは散乱X線)を検出す
る形式の走査X線顕微鏡において試料表面の凹凸に起因
するコントラストを生成することが出来るので、試料表
面形状を測定出来るという効果がある。ADVANTAGE OF THE INVENTION According to this invention, since the contrast resulting from the unevenness | corrugation of a sample surface can be produced | generated in the scanning X-ray microscope of the type which detects fluorescence (or scattered X-ray), there exists an effect that a sample surface shape can be measured.
第1図は本発明の原理を示す側面図、第2図は本発明の
一実施例のX線顕微鏡の側面図である。 1…試料、2……X線検出器、3…試料に入射するマイ
クロX線ビーム、4…試料から放射される蛍光(あるい
は散乱)X線、5…X線発生装置、6…X線集光鏡、7
…試料走査機構、8…計測画像処理計算機、9…デイス
プレイ。FIG. 1 is a side view showing the principle of the present invention, and FIG. 2 is a side view of an X-ray microscope according to one embodiment of the present invention. DESCRIPTION OF SYMBOLS 1 ... Sample, 2 ... X-ray detector, 3 ... Micro X-ray beam incident on sample, 4 ... Fluorescent (or scattered) X-ray emitted from sample, 5 ... X-ray generator, 6 ... X-ray collection Light mirror, 7
... sample scanning mechanism, 8 ... measurement image processing computer, 9 ... display.
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭62−106352(JP,A) 特開 昭60−76652(JP,A) 特開 平1−232647(JP,A) 内田、重田、鈴木、「走査型X線顕微 鏡によるGaAsFETの素子構造の観 察」、精密工学会誌、58巻、3号、546 −551ページ (58)調査した分野(Int.Cl.6,DB名) G21K 7/00 JICSTファイル(JOIS)────────────────────────────────────────────────── ─── Continuation of the front page (56) References JP-A-62-106352 (JP, A) JP-A-60-76652 (JP, A) JP-A-1-232647 (JP, A) Uchida, Shigeta, Suzuki , “Observation of GaAsFET device structure with scanning X-ray microscope”, Journal of the Japan Society of Precision Engineering, Vol. 58, No. 3, pp. 546-551 (58) Fields investigated (Int. Cl. 6 , DB name) G21K7 / 00 JICST file (JOIS)
Claims (1)
光X線あるいは散乱X線検出器及び検出信号を画像とし
て表示する画像表示器から成る走査型X線顕微鏡装置に
おいて、X線を放射するX線発生装置と、前記X線を反
射して細く絞ったX線ビームとするX線集光鏡とを有
し、細く絞ったX線ビームを試料表面にほぼ垂直に入射
させ、さらに蛍光(あるいは散乱)X線の検出角度にお
いて試料面に対して浅い角度に放射される部分のなかで
もさらに所望とする特定の方向に放射されるものを表示
信号とすることを特徴とする走査型X線顕微鏡。1. A scanning X-ray microscope apparatus comprising a finely focused X-ray beam, a sample scanning mechanism, a fluorescent X-ray or scattered X-ray detector, and an image display for displaying a detection signal as an image. An X-ray generator that reflects the X-rays, and an X-ray focusing mirror that reflects the X-rays to convert the X-ray into a finely focused X-ray beam. Scanning X-rays, characterized in that, among the portions radiated at a shallow angle with respect to the sample surface at the X-ray detection angle, those radiated in a desired specific direction are used as display signals. Line microscope.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8790789A JP2901637B2 (en) | 1989-04-10 | 1989-04-10 | Scanning X-ray microscope |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8790789A JP2901637B2 (en) | 1989-04-10 | 1989-04-10 | Scanning X-ray microscope |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02268300A JPH02268300A (en) | 1990-11-01 |
| JP2901637B2 true JP2901637B2 (en) | 1999-06-07 |
Family
ID=13927985
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8790789A Expired - Lifetime JP2901637B2 (en) | 1989-04-10 | 1989-04-10 | Scanning X-ray microscope |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2901637B2 (en) |
-
1989
- 1989-04-10 JP JP8790789A patent/JP2901637B2/en not_active Expired - Lifetime
Non-Patent Citations (1)
| Title |
|---|
| 内田、重田、鈴木、「走査型X線顕微鏡によるGaAsFETの素子構造の観察」、精密工学会誌、58巻、3号、546−551ページ |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02268300A (en) | 1990-11-01 |
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