EP2461332B1 - Convertisseur point-trait - Google Patents
Convertisseur point-trait Download PDFInfo
- Publication number
- EP2461332B1 EP2461332B1 EP11191307.5A EP11191307A EP2461332B1 EP 2461332 B1 EP2461332 B1 EP 2461332B1 EP 11191307 A EP11191307 A EP 11191307A EP 2461332 B1 EP2461332 B1 EP 2461332B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- ray
- source
- sample
- configuration according
- optical element
- 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.)
- Active
Links
- 230000003287 optical effect Effects 0.000 claims description 19
- 238000002441 X-ray diffraction Methods 0.000 claims description 5
- 229910001338 liquidmetal Inorganic materials 0.000 claims description 2
- 230000005855 radiation Effects 0.000 claims description 2
- 238000002474 experimental method Methods 0.000 description 3
- 238000006243 chemical reaction Methods 0.000 description 2
- 239000013078 crystal Substances 0.000 description 2
- 239000000919 ceramic Substances 0.000 description 1
- 230000003750 conditioning effect Effects 0.000 description 1
- 238000002050 diffraction method Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000002241 glass-ceramic Substances 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 239000002086 nanomaterial Substances 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- 238000002310 reflectometry Methods 0.000 description 1
- 230000011514 reflex Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 235000012431 wafers Nutrition 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K1/00—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating
- G21K1/06—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diffraction, refraction or reflection, e.g. monochromators
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K2201/00—Arrangements for handling radiation or particles
- G21K2201/06—Arrangements for handling radiation or particles using diffractive, refractive or reflecting elements
- G21K2201/064—Arrangements for handling radiation or particles using diffractive, refractive or reflecting elements having a curved surface
Definitions
- the invention relates to an X-ray optical arrangement for illuminating a sample with an X-ray beam which has a line-shaped cross-section, the arrangement comprising an X-ray source and a beam-conditioning X-ray optics.
- X-ray diffraction generates interferences (reflections) on three-dimensional periodic structures on the atomic scale (crystals) according to Bragg's law.
- the angular position of the reflexes and their intensity contain important information about the atomic and microstructure of the substances to be investigated.
- Point sources are used in X-ray diffractometry when it comes to examining point-like objects, such as small crystals with edge lengths of 10 to 100 microns, or when measuring on larger sample surfaces such as semiconductor wafers with local resolution down to a few 10 microns square.
- stroke sources are used if you want to examine larger sample surfaces. This is typical of the use of Bragg-Brentano geometry to detect crystalline phases in a sample, but also in high-resolution diffractometry and reflectometry.
- the use of line sources usually has two advantages: firstly, the electrons coming from the cathode and thus the current are distributed over a larger area on the anode (for example, 0.4 ⁇ 12 mm 2 in a long-fine-focus tube). Thus, typically a very high power can be impressed without the anode melting due to the heat load.
- the second advantage arises from the fact that the x-ray beam is usually taken at an angle from the anode, which is about 6 ° in commercial metal-ceramic tubes. As a result, the visible focal spot is only 0.04 x 12 mm 2 , and just the 0.04 mm affect the fact that the obtained angular resolution in the diffraction experiment is much better than comparable point sources.
- the 0.4 x 12 mm 2 x-ray tube has a second radiolucent window, 90 ° to the line focus window. Below 6 ° Abgriffwinkel then the focal spot is 0.4 x 1.2 mm 2 large.
- the X-ray flux is exactly as large as through the window for the line focus, but the larger extension of the focal spot in the x-direction, the angular resolution in the experiment is significantly worse.
- Point sources that would provide a comparable resolution as the line source would have to have a focal point of about 0.04 x 0.04 mm 2 . These are microfocus sources, but they only work at 50 W because otherwise the surface load of electrons would melt the anode.
- microstructures and nanostructures with the aid of X-ray diffractometry must be converted with standard X-ray diffractometers between line focus and point focus sources.
- X-ray diffractometers between line focus and point focus sources.
- Such a conversion is extremely complicated and time-consuming, since either in glass-ceramic tubes, the X-ray tube must be rotated or need to be changed in rotary anodes cathode, filament and installation direction. Accordingly, the associated optics must be exchanged and usually re-adjusted consuming. This hinders in particular the use of microfocus sources or other brilliant x-ray sources.
- the present invention is intended to make it possible to use both point and line-shaped beam geometries without a complicated and time-consuming conversion must be made.
- the X-ray source is a brilliant point source
- the X-ray optics comprises an X-ray optical element with a Kirkpatrick-Baez or a Montel mirror arrangement, which conditions X-ray light emanating from the point source, in that the X-ray beam is parallelized with respect to a direction perpendicular to the beam propagation direction and remains divergent with respect to a direction perpendicular thereto and to the beam propagation direction, and which is rotatable about the axis of the beam propagation direction.
- the X-ray optical element is rotatable about the axis of the beam propagation direction by 90 °.
- a further embodiment is characterized in that the brilliant point source comprises a rotary anode or a microfocus source or a liquid-metal arrangement.
- a diaphragm is arranged in the region of the sample, which blanks the X-ray beam with a line-shaped cross-sectional profile onto a beam profile with punctiform beam cross-section.
- X-ray optics consists of the X-ray optical element.
- an embodiment is preferable in which a monochromator is interposed between the X-ray optical element and the sample.
- the invention also includes an X-ray optical element which is suitable for use in an X-ray optical arrangement according to the invention and is characterized in that the X-ray optical element can image a point on a line focus.
- an X-ray analysis device with an X-ray optical arrangement according to the invention is required.
- Fig. 1 the device according to the invention is shown schematically.
- the representation corresponds to a section in the longitudinal direction through the device according to the invention.
- the sample 1 is illuminated by X-ray light which propagates from the X-ray source 2 through the X-ray optical element 3 according to the invention.
- the X-ray source 2 comprises a brilliant point source 4.
- Fig. 1 Two mutually perpendicular planes are in Fig. 1 shown.
- level 1 the beam paths of the X-ray light leaving the X-ray optical element 3 are parallel.
- plane 2 perpendicular thereto, the beam paths of the X-ray light leaving the X-ray optical element 3 are divergent. This results in the location of the sample 1, a line-shaped form of the beam.
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- High Energy & Nuclear Physics (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
Claims (7)
- Dispositif optique à rayons X pour éclairer un échantillon (1) avec un faisceau de rayons X qui présente une section transversale en forme de trait, lequel dispositif contient une source de rayons X (2) ainsi qu'une optique à rayons X pour conditionner le faisceau,
caractérisé en ce
que la source de rayons X (2) comprend une source ponctuelle brillante (4),
et que l'optique à rayons X comprend un élément optique à rayons X (3) avec un système de miroirs Kirkpatrick-Baez ou Montel, lequel conditionne les rayons X provenant de la source ponctuelle de façon que le faisceau de rayons X soit parallélisé par rapport à une direction perpendiculaire à la direction de propagation du faisceau et reste divergent par rapport à une direction perpendiculaire à celle-ci ainsi qu'à la direction de propagation du faisceau, et lequel peut tourner autour de l'axe de la direction de propagation du faisceau. - Dispositif selon la revendication 1, caractérisé en ce qu'il s'applique 1 ≤ AQ ≤ 1,5 pour le rapport d'aspect AQ de la source ponctuelle et AS ≥ 2 pour le rapport d'aspect AS de la section transversale du faisceau dans la zone de l'échantillon (1).
- Dispositif selon l'une des revendications précédentes, caractérisé en ce que la source ponctuelle brillante (4) comprend une anode tournante, une source à microfoyer ou un dispositif à métal liquide.
- Dispositif selon l'une des revendications précédentes, caractérisé en ce que dans la zone de l'échantillon (1) est disposé un diaphragme qui diaphragme le faisceau de rayons X à profil de section transversale en forme de trait en un profil de faisceau à section transversale en forme de point.
- Dispositif selon l'une des revendications 1 à 4, caractérisé en ce que l'optique à rayons X est constituée de l'élément optique à rayons X (3).
- Dispositif selon l'une des revendications 1 à 4, caractérisé en ce qu'un monochromateur est disposé entre l'élément optique à rayons X (3) et l'échantillon (1).
- Appareil d'analyse à rayons X doté d'un dispositif optique à rayons X selon l'une des revendications précédentes.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE201010062472 DE102010062472A1 (de) | 2010-12-06 | 2010-12-06 | Punkt-Strich-Konverter |
Publications (2)
Publication Number | Publication Date |
---|---|
EP2461332A1 EP2461332A1 (fr) | 2012-06-06 |
EP2461332B1 true EP2461332B1 (fr) | 2016-07-27 |
Family
ID=45044441
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP11191307.5A Active EP2461332B1 (fr) | 2010-12-06 | 2011-11-30 | Convertisseur point-trait |
Country Status (3)
Country | Link |
---|---|
US (1) | US8848870B2 (fr) |
EP (1) | EP2461332B1 (fr) |
DE (1) | DE102010062472A1 (fr) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2013184999A1 (fr) | 2012-06-08 | 2013-12-12 | Rigaku Innovative Technologies, Inc. | Caméra à diffusion à petit angle double mode |
CA2875682A1 (fr) | 2012-06-08 | 2013-12-12 | Rigaku Innovative Technologies, Inc. | Systeme a faisceau de rayons x offrant des faisceaux monodimensionnel (1d) et bidimensionnel (2d) |
US10352881B2 (en) * | 2016-12-27 | 2019-07-16 | Malvern Panalytical B.V. | Computed tomography |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20040190681A1 (en) * | 2003-03-26 | 2004-09-30 | Rigaku Corporaton | X-ray diffraction apparatus |
Family Cites Families (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE19833524B4 (de) | 1998-07-25 | 2004-09-23 | Bruker Axs Gmbh | Röntgen-Analysegerät mit Gradienten-Vielfachschicht-Spiegel |
US6703406B2 (en) | 1999-07-30 | 2004-03-09 | University Of Kentucky Research Foundation | 2,6-disubstituted piperidines as modulators of nicotinic acetylcholine receptor mediated neurotransmitter release, uptake and storage |
US6282259B1 (en) * | 1999-09-10 | 2001-08-28 | Rigaku/Msc, Inc. | X-ray mirror system providing enhanced signal concentration |
DE10107914A1 (de) * | 2001-02-14 | 2002-09-05 | Fraunhofer Ges Forschung | Anordnung für röntgenanalytische Anwendungen |
DE10160472B4 (de) * | 2001-12-08 | 2004-06-03 | Bruker Axs Gmbh | Röntgen-optisches System und Verfahren zur Abbildung einer Strahlungsquelle |
DE10162093A1 (de) * | 2001-12-18 | 2003-07-10 | Bruker Axs Gmbh | Röntgen-optisches System mit Blende im Fokus einer Röntgen-Spiegels |
KR100576921B1 (ko) | 2003-01-15 | 2006-05-03 | 한국원자력연구소 | 고광도의 평행빔 생성 장치 |
EP1477795B1 (fr) * | 2003-05-14 | 2007-03-14 | Bruker AXS GmbH | Diffractomètre à rayons X pour la diffraction à incidence rasante d'échantillons orientés horizontalement et verticalement |
DE102006015933B3 (de) | 2006-04-05 | 2007-10-31 | Incoatec Gmbh | Vorrichtung und Verfahren zum Justieren eines optischen Elements |
DE102008050851B4 (de) * | 2008-10-08 | 2010-11-11 | Incoatec Gmbh | Röntgenanalyseinstrument mit verfahrbarem Aperturfenster |
-
2010
- 2010-12-06 DE DE201010062472 patent/DE102010062472A1/de not_active Ceased
-
2011
- 2011-11-23 US US13/373,644 patent/US8848870B2/en active Active
- 2011-11-30 EP EP11191307.5A patent/EP2461332B1/fr active Active
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20040190681A1 (en) * | 2003-03-26 | 2004-09-30 | Rigaku Corporaton | X-ray diffraction apparatus |
Also Published As
Publication number | Publication date |
---|---|
US20120140897A1 (en) | 2012-06-07 |
DE102010062472A1 (de) | 2012-06-06 |
US8848870B2 (en) | 2014-09-30 |
EP2461332A1 (fr) | 2012-06-06 |
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