JPS5590847A - Xxray spectroscope - Google Patents
Xxray spectroscopeInfo
- Publication number
- JPS5590847A JPS5590847A JP16359878A JP16359878A JPS5590847A JP S5590847 A JPS5590847 A JP S5590847A JP 16359878 A JP16359878 A JP 16359878A JP 16359878 A JP16359878 A JP 16359878A JP S5590847 A JPS5590847 A JP S5590847A
- Authority
- JP
- Japan
- Prior art keywords
- spectral
- parts
- single crystal
- lolland
- curved single
- 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.)
- Granted
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
- G01N23/2076—Diffractometry using detectors, e.g. using a probe in a central position and one or more displaceable detectors in circumferential positions for spectrometry, i.e. using an analysing crystal, e.g. for measuring X-ray fluorescence spectrum of a sample with wavelength-dispersion, i.e. WDXFS
-
- 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
- G01N23/22—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 measuring secondary emission from the material
- G01N23/223—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 measuring secondary emission from the material by irradiating the sample with X-rays or gamma-rays and by measuring X-ray fluorescence
Landscapes
- Chemical & Material Sciences (AREA)
- Physics & Mathematics (AREA)
- General Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Dispersion Chemistry (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Crystallography & Structural Chemistry (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
Abstract
PURPOSE:To make it possible to cubically condense characteristic X-rays irradiated by dividing the spectral face of a curved single crystal into a plurality parts in the thickness direction perpendicular to the Lolland circle plane, and providing these parts at specific positions corresponding to the specific wavelength to be spectral- diffracted. CONSTITUTION:The spectral face of a curved single crystal is divided into a plurality parts, for example, three parts 7-9 in the thickness direction perpendiculor to the Lolland circle 6 plane. In correspondence to the specific wavelength of characteristic X-rays to be spectral-diffracted, these parts are positioned, in contacting manner, at rotating curvature formed by rotating the condensing curve of the spectral face of the curved single crystal 4 around the axis of a straight line connecting the focal point S and X-ray source P moving on the Lolland circle 6. By this procedure, the spectral face of the curved single crystal which has not been useful for condensation in the conventional device is made usable, and it is possible to obtain an X-ray spectroscope close to the complete condensation type capable of condensing cubic characteristic X-rays.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16359878A JPS5590847A (en) | 1978-12-29 | 1978-12-29 | Xxray spectroscope |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16359878A JPS5590847A (en) | 1978-12-29 | 1978-12-29 | Xxray spectroscope |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5590847A true JPS5590847A (en) | 1980-07-09 |
JPS6259257B2 JPS6259257B2 (en) | 1987-12-10 |
Family
ID=15776956
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16359878A Granted JPS5590847A (en) | 1978-12-29 | 1978-12-29 | Xxray spectroscope |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5590847A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6161456U (en) * | 1984-09-28 | 1986-04-25 | ||
US5569919A (en) * | 1994-10-04 | 1996-10-29 | Kabushiki Kaisha Kobe Seiko Sho | X-ray analytical apparatus |
-
1978
- 1978-12-29 JP JP16359878A patent/JPS5590847A/en active Granted
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6161456U (en) * | 1984-09-28 | 1986-04-25 | ||
JPH0512762Y2 (en) * | 1984-09-28 | 1993-04-02 | ||
US5569919A (en) * | 1994-10-04 | 1996-10-29 | Kabushiki Kaisha Kobe Seiko Sho | X-ray analytical apparatus |
Also Published As
Publication number | Publication date |
---|---|
JPS6259257B2 (en) | 1987-12-10 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JPS5437077A (en) | Chemical evaporation method and apparatus for same | |
JPS5590847A (en) | Xxray spectroscope | |
JPS5351540A (en) | Sun tracking device | |
JPS533879A (en) | Thermometer by infrared-ray radiation | |
JPS52147449A (en) | Optical branching and condensing devices | |
JPS5389791A (en) | X-ray spectroscope | |
JPS559507A (en) | Focal plane shutter of blade type | |
JPS56112616A (en) | Spectroscope with concave diffraction grating | |
JPS5341184A (en) | Ion injection device | |
JPS52140348A (en) | Optical device for photo-processing | |
GB2008203A (en) | Rotor Blade Fixing | |
LABEYRIE et al. | Holo-gratings and spectrograph design(Holographic gratings for spectrometers noting luminosity and concave stigmatism) | |
SCHMAHL et al. | Stellar spectroscopy with holographic gratings(Holographic gratings for stellar spectroscopy) | |
JPS5291291A (en) | Method for marking propeller vanes | |
JPS53137353A (en) | Center of axis positioning and its device | |
Kostishin et al. | Exciton absorption band splitting in the PbI 2 spectrum | |
SU628197A1 (en) | Composition for obtaining fibrous material | |
JPS5359391A (en) | X-ray generator | |
JPS51148442A (en) | Mode-distribution analytical method | |
JPS548571A (en) | Pressure measuring device | |
JPS53135374A (en) | X-ray stress measuring device | |
SU678637A1 (en) | Phase distinguishing device | |
JPS578422A (en) | Oblique incident spectroscope | |
JPS5643520A (en) | Concave surface diffraction grating spectrometer | |
JPS5369764A (en) | Inner edge for a reciprocal electric razor |