JPH0330101B2 - - Google Patents
Info
- Publication number
- JPH0330101B2 JPH0330101B2 JP55152905A JP15290580A JPH0330101B2 JP H0330101 B2 JPH0330101 B2 JP H0330101B2 JP 55152905 A JP55152905 A JP 55152905A JP 15290580 A JP15290580 A JP 15290580A JP H0330101 B2 JPH0330101 B2 JP H0330101B2
- Authority
- JP
- Japan
- Prior art keywords
- rays
- ray
- spectroscopic
- measured
- wavelength
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N23/00—Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
- G01N23/20—Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by using diffraction of the radiation by the materials, e.g. for investigating crystal structure; by using scattering of the radiation by the materials, e.g. for investigating non-crystalline materials; by using reflection of the radiation by the materials
- G01N23/207—Diffractometry using detectors, e.g. using a probe in a central position and one or more displaceable detectors in circumferential positions
Landscapes
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
Description
【発明の詳細な説明】
この発明は、従来、特定波長およびその整数倍
波長のみを取り出すために用いられてきたX線分
光結晶に微小回転振動を与えることによつて、分
光波長に一定の周期の変調をかけ、位相敏感検出
法によりX線回折、散乱、吸収等の測定を精度良
く行うことができるようにしたX線測定方法に関
するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a constant periodicity to spectral wavelengths by applying minute rotational vibrations to an X-ray spectroscopy crystal, which has conventionally been used to extract only a specific wavelength and its integral multiple wavelength. The present invention relates to an X-ray measurement method in which X-ray diffraction, scattering, absorption, etc. can be measured with high accuracy by modulating the X-rays using a phase-sensitive detection method.
一般に結晶のブラツグ反射を利用した分光原理
は、連続波長(白色)X線の中から下記第(1)式を
満足するような特定の波長およびその整数倍波長
を選びだすことに基づいている。 In general, the principle of spectroscopy that utilizes the Bragg reflection of crystals is based on selecting a specific wavelength and its integral multiples that satisfy the following equation (1) from among continuous wavelength (white) X-rays.
2dok1・sinθp=nλ ……(1)
ここに、θp:hk1反射のブラツグ角
dok1:hk1面の面間隔
λ:1次反射によるX線の波長
ここでさらに分光結晶を微小各δθだけ回転した
とすれば、波長変化は下記第(2)式で近似的に表す
ことができる。 2d ok1・sinθ p = nλ ……(1) Here, θ p : Bragg angle of hk1 reflection d ok1 : Interplanar spacing of hk1 plane λ : Wavelength of X-ray due to primary reflection Here, the spectroscopic crystal is further divided into minute δθ The wavelength change can be approximately expressed by the following equation (2).
Δλ〜2dhk1cosθpsinδθ ……(2)
(δθ≪1であることを用いた)
もし、δθを各周波数ωで正弦関数的に動かすな
らば、δθに基づく波長変化はδθ≪1から、下記第
(3)式で表わすことができる。 Δλ〜2d hk1 cosθ p sinδθ ...(2) (using the fact that δθ≪1) If δθ is moved sinusoidally at each frequency ω, the wavelength change based on δθ is from δθ≪1, Part below
It can be expressed by equation (3).
Δλ〜2dhk1Asin(ωt+α) ……(3)
ここに、A:δθの振幅
α:δθの位相
第(3)式から波長変化Δλが正弦関数で表わすこ
とができることを示している。 Δλ~2d hk1 Asin(ωt+α) (3) where A: amplitude of δθ α: phase of δθ Equation (3) shows that the wavelength change Δλ can be expressed by a sine function.
この発明は上記の原理に基づいてなされたもの
である。以下、この発明を図面を用いて説明す
る。 This invention has been made based on the above principle. Hereinafter, this invention will be explained using the drawings.
第1図はこの発明の一実施例における分光結晶
部を示したものである。この図で1はX線源、
2,2′は分光結晶で、回転台3上に取り付けら
れており、分光結晶2,2′の間隔をDとする。
両結晶2,2′は分光系を構成しており、X線源
1からの平行なX線の入射点を中心に分光結晶
2,2′が回転することによつて、第(1)式を満足
するような波長のX線のみ(一般にはnλ、n=
1,2,……であるが、簡単のためここでは高次
項を無視して説明する)、入射光と平行に反射す
る。あるブラツグ角θpの近傍で、微小角δθだけ微
小回転が加わつたとすると、分光結晶2はOAか
らOA′に傾き、反射X線経路はOPからOP′に変
わる。 FIG. 1 shows a spectroscopic crystal section in one embodiment of the present invention. In this figure, 1 is an X-ray source,
Reference numerals 2 and 2' designate spectroscopic crystals, which are mounted on the rotary table 3, and the distance between the spectroscopic crystals 2 and 2' is D.
Both crystals 2 and 2' constitute a spectroscopic system, and by rotating the spectroscopic crystals 2 and 2' around the incident point of parallel X-rays from the X-ray source 1, the equation (1) Only X-rays with wavelengths that satisfy (generally nλ, n=
1, 2, ..., but for the sake of simplicity, higher-order terms will be ignored here), and are reflected in parallel to the incident light. If a minute rotation is applied by a minute angle δθ near a certain Bragg angle θ p , the spectroscopic crystal 2 will tilt from OA to OA', and the reflected X-ray path will change from OP to OP'.
この時第(2)式で表される波長変調を受けた波長
λ′(=λ+Δλ)のX線を入射X線と平行に取り出
すことができる。この波長変調に検出系の位相を
同期させることによつて、変調X線分光測定およ
び変調X線回折が可能となる。 At this time, an X-ray having a wavelength λ' (=λ+Δλ) that has undergone wavelength modulation expressed by equation (2) can be extracted in parallel to the incident X-ray. By synchronizing the phase of the detection system with this wavelength modulation, modulated X-ray spectrometry and modulated X-ray diffraction become possible.
上記はこの発明の原理であるが、これを利用し
たこの発明のX線測定方法を実施する装置の一例
を第2図のブロツク図に示す。 The above is the principle of the present invention, and an example of an apparatus for carrying out the X-ray measurement method of the present invention using the principle is shown in the block diagram of FIG.
第2図において、11はX線源、12は分光結
晶微小回転振動装置、13は被測定試料、14は
X線検出器、15は位相敏感検出器、16は微小
回転駆動源である。上記位相敏感検出器15は、
時間軸に対して変動する物理量を位相信号(参照
信号と呼ばれる)に同期させて測定する装置をさ
す。具体的には微小電流測定に用いられるロツク
インアンプが代表的な例であるが、この発明にお
いてはX線検出器に参照信号に同期したゲートを
かけデイジタル方式のロツクイン測定を行う。参
照信号は微小回転駆動源16、例えばピエゾ素子
に加える正弦波信号を用いる。 In FIG. 2, 11 is an X-ray source, 12 is a spectroscopic crystal microrotation vibration device, 13 is a sample to be measured, 14 is an X-ray detector, 15 is a phase sensitive detector, and 16 is a microrotation drive source. The phase sensitive detector 15 is
A device that measures physical quantities that vary with respect to the time axis by synchronizing them with a phase signal (called a reference signal). Specifically, a typical example is a lock-in amplifier used for microcurrent measurement, but in the present invention, a digital lock-in measurement is performed by applying a gate to an X-ray detector in synchronization with a reference signal. As the reference signal, a sine wave signal applied to the minute rotational drive source 16, for example a piezo element, is used.
この発明の要旨はX線の位相敏感検出を波長変
調法と組み合わせることによつてX線回折および
吸収測定の高精度化を図ることである。 The gist of this invention is to improve the precision of X-ray diffraction and absorption measurements by combining phase-sensitive detection of X-rays with a wavelength modulation method.
その動作を説明すると、X線源11より出た連
続X線を、角周波数ωで回転振動している分光結
晶微小回転振動装置12に入射させて波長変調を
加えた後、被測定試料13に照射し、被測定試料
13により回折・散乱させたX線をX線検出器1
4で検出する。このX線検出器14の出力を微小
回転駆動源16の出力を参照信号として位相敏感
検出器15により測定する。これにより被測定試
料13によるX線回折・散乱を信号対雑音比良く
測定することができる。 To explain its operation, the continuous X-rays emitted from the X-ray source 11 are made incident on the spectroscopic crystal micro-rotary oscillator 12 that rotates at an angular frequency ω, and after wavelength modulation is applied to the sample 13 to be measured. The X-ray detector 1 transmits the X-rays that are irradiated and diffracted and scattered by the sample to be measured 13.
4 to detect. The output of this X-ray detector 14 is measured by a phase sensitive detector 15 using the output of the minute rotation drive source 16 as a reference signal. Thereby, X-ray diffraction and scattering by the sample to be measured 13 can be measured with a good signal-to-noise ratio.
すなわち、位相敏感検出器15は不規則な雑音
から一定の規則性を持つ信号を取り出す作用をす
る。この発明で対象とするのは表面や薄膜等信号
強度が弱く通常の測定では雑音に埋もれてしまう
ような場合に威力を発揮する。位相に対して規則
性を持つ信号を取り出して積算することにより信
号対雑音比を向上させることができる。 That is, the phase sensitive detector 15 functions to extract a signal with a certain regularity from irregular noise. This invention is effective in cases where the signal strength is weak and would be buried in noise in normal measurements, such as on surfaces or thin films. The signal-to-noise ratio can be improved by extracting and integrating signals that have regularity with respect to phase.
以上説明したように、この発明はブラツグ反射
を利用して特定波長またはその整数倍の波長の分
光X線を得てそれを用いてX線測定を行う方法で
あつて、分光結晶に微小回転振動を与えて分光X
線に変調を加え、この変調された分光X線を用い
たので、バツクグラウンドを効果的に除くことが
でき、信号対雑音比が向上するため任意の入射X
線波長で精度のよいX線回折・散乱データを得る
ことができる利点がある。 As explained above, the present invention is a method of obtaining spectroscopic X-rays of a specific wavelength or an integer multiple thereof using Bragg reflection, and performing X-ray measurements using the spectroscopic X-rays. Spectral X by giving
By modulating the X-rays and using the modulated spectroscopic X-rays, the background can be effectively removed and the signal-to-noise ratio is improved.
It has the advantage of being able to obtain highly accurate X-ray diffraction/scattering data at line wavelengths.
第1図はこの発明の動作原理の説明図、第2図
はこの発明の一実施例の実施に用いるX線測定装
置の一例を示すブロツク図である。
図中、1,11はX線源、2,2′は分光結晶、
3は回転台、12は分光結晶微小回転振動装置、
13は被測定試料、14はX線検出器、15は位
相敏感検出器、16は微小回転駆動源である。
FIG. 1 is an explanatory diagram of the operating principle of the present invention, and FIG. 2 is a block diagram showing an example of an X-ray measuring apparatus used for carrying out an embodiment of the present invention. In the figure, 1 and 11 are X-ray sources, 2 and 2' are spectroscopic crystals,
3 is a rotary table, 12 is a spectroscopic crystal micro-rotation vibration device,
13 is a sample to be measured, 14 is an X-ray detector, 15 is a phase sensitive detector, and 16 is a minute rotation drive source.
Claims (1)
記分光結晶によるX線のフラツグ反射を利用して
特定波およびその整数倍の波長の単色X線を得る
際に、前記分光結晶に分光結晶微小回転振動装置
により微小回転振動を与え前記単色X線の入射点
を中心に平行な2枚の分光結晶が回転することに
より前記単色X線に波長変調を加えた後、被測定
試料に照射し、前記被測定試料により回折・散乱
されたX線をX線検出器で検出し、一方、前記微
小回転振動源の出力を参照信号として位相敏感検
出器により前記X線検出器からのX線のX線回
折、散乱または吸収スペクトルの測定を行うこと
を特徴とするX線測定方法。1 When two parallel spectroscopic crystals are rotated by a small angle and monochromatic X-rays of a specific wave and a wavelength of an integral multiple thereof are obtained by using the flag reflection of X-rays by the spectroscopic crystal, the spectroscopic crystal is attached to the spectroscopic crystal. Micro-rotational vibration is applied by a micro-rotary vibration device, and two parallel spectroscopic crystals are rotated around the point of incidence of the monochromatic X-rays, thereby adding wavelength modulation to the monochromatic X-rays, and then irradiating the sample to be measured. , the X-rays diffracted and scattered by the sample to be measured are detected by an X-ray detector, and the X-rays from the X-ray detector are detected by a phase-sensitive detector using the output of the micro-rotational vibration source as a reference signal. An X-ray measurement method characterized by measuring X-ray diffraction, scattering, or absorption spectra.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55152905A JPS5776441A (en) | 1980-10-30 | 1980-10-30 | Modulation method for x-ray wavelength |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55152905A JPS5776441A (en) | 1980-10-30 | 1980-10-30 | Modulation method for x-ray wavelength |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5776441A JPS5776441A (en) | 1982-05-13 |
| JPH0330101B2 true JPH0330101B2 (en) | 1991-04-26 |
Family
ID=15550692
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55152905A Granted JPS5776441A (en) | 1980-10-30 | 1980-10-30 | Modulation method for x-ray wavelength |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5776441A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| RU2642886C1 (en) * | 2016-11-30 | 2018-01-29 | Федеральное государственное автономное образовательное учреждение высшего образования "Национальный исследовательский Нижегородский государственный университет им. Н.И. Лобачевского" | Intensity modulation of x-ray beam |
| CN107219241B (en) | 2017-05-05 | 2020-10-16 | 中国科学院上海光学精密机械研究所 | In-situ time-resolved X-ray absorption spectrum measurement device and measurement method |
-
1980
- 1980-10-30 JP JP55152905A patent/JPS5776441A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5776441A (en) | 1982-05-13 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| RU2012872C1 (en) | Method for obtaining image of object internal structure | |
| JP3337734B2 (en) | Infrared ellipsometer | |
| CN1841030B (en) | Spectroscopic polarimetry | |
| JPH08128971A (en) | Exafs measuring device | |
| JP3311497B2 (en) | Fourier transform spectral phase modulation ellipsometry | |
| JPH0330101B2 (en) | ||
| CA1048806A (en) | Rotating-compensator ellipsometer | |
| KR100380766B1 (en) | Method for evaluating displaying element of liquid crystal, information storage medium for storing computer program representative of the method and evaluating system using the same | |
| JP3029757B2 (en) | Sample evaluation method by photothermal displacement measurement | |
| US4167338A (en) | Method and apparatus for determining the quantity ratio of two components of a multi-substance mixture | |
| JPH06288835A (en) | Ellipsometer | |
| JP3250272B2 (en) | Birefringence measurement method and device | |
| JP2001033406A (en) | X-ray phase difference image pickup method and device | |
| US7046373B2 (en) | Interferometric system for the simultaneous measurement of the index of refraction and of the thickness of transparent materials, and related procedure | |
| SU522458A1 (en) | X-ray three-crystal spectrometer | |
| JPH02500541A (en) | Method for measuring the concentration of a gas in a gas mixture and apparatus for carrying out this method | |
| JP2000221147A (en) | Crystal orientation angle measurement device and method | |
| CN110596013B (en) | High-optical-rotation-rate material optical rotation rate detection device | |
| SU1140009A1 (en) | Ellipsometric spectroscopy method | |
| JP2580943B2 (en) | Measuring method for unevenness of single crystal substrate | |
| SU1087853A1 (en) | Surface machining quality control method | |
| SU1081434A1 (en) | Method of measuring polarization degree | |
| JP2568653B2 (en) | Ellipsometer | |
| SU1702265A1 (en) | Method of precision measurement of periods of crystal lattice | |
| JPS62137541A (en) | Diffusive reflection measurement |