阅读说明：本技术 光学镜、x射线荧光分析装置以及x射线荧光分析方法 (Optical mirror, X-ray fluorescence analysis device, and X-ray fluorescence analysis method ) 是由 V·勒西格 于 2014-02-27 设计创作，主要内容包括：本发明涉及一种用于X射线荧光分析装置,包括X射线源(10),用来利用X射束(19)辐照试样(15)；X射线探测器(17),用于测量由所述试样(15)发出的X射线荧光辐射(16)；以及摄像机(25),用于经由光学镜(20)产生试样(15)的被辐照的测量位置(29)的光学控制图像(26),所述光学镜在所述X射线源(10)的射束路径中成角度地布置,所述光学镜包括载体(21),在所述载体(21)上设置有镜层(28)。为了创建X射线荧光装置,由其真实控制记录待分析试样、尤其采用的表面点是可行的,本发明提供了光学镜(20)具有用于X射束(19)的通窗(23),其由载体(21)中的开口(23)以及形成镜层(28)的膜(22)形成,所述膜在载体(21)的外表面上覆盖开口(23)。(The invention relates to an apparatus for X-ray fluorescence analysis, comprising an X-ray source (10) for irradiating a sample (15) with an X-ray beam (19); an X-ray detector (17) for measuring X-ray fluorescence radiation (16) emitted by the sample (15); and a camera (25) for generating an optically controlled image (26) of the irradiated measurement location (29) of the sample (15) via an optical mirror (20) which is arranged angularly in the beam path of the X-ray source (10), the optical mirror comprising a carrier (21) on which a mirror layer (28) is arranged. In order to create an X-ray fluorescence apparatus, from the actual control of which it is possible to record the sample to be analyzed, in particular the surface points used, the invention provides that the optical mirror (20) has a through-window (23) for the X-ray beam (19), which is formed by an opening (23) in the carrier (21) and a film (22) forming a mirror layer (28), which covers the opening (23) on the outer surface of the carrier (21).)

1. An optical mirror for an X-ray fluorescence analysis apparatus having an X-ray source (10) for irradiating a sample (15) with an X-ray beam (19); an X-ray detector (17) for measuring X-ray fluorescence radiation (16) emitted by the sample; and a camera (25) for generating an optically controlled image (26) of the irradiated measurement location (29) of the sample (15) via the optical mirror (20), which is arranged angularly in the beam path of the X-ray source (10), which optical mirror comprises a carrier (21), on which carrier (21) a mirror layer (28) is provided,

it is characterized in that the preparation method is characterized in that,

the carrier (21) has a flat base body which has a recess (23) in the region of the through-window for the X-ray beam (19), and a film (22) which covers the flat base body and the recess (23) forms the mirror layer (28) on the outside of the carrier (21), wherein the film (22) is bonded to the carrier (21) and covers the recess (23) of the carrier (21) in a tensionless manner, and wherein the flat base body is made of glass.

2. The optical mirror according to claim 1, characterized in that the membrane (22) is made of plastic.

3. An optical mirror according to claim 2, characterized in that the film (22) is made of polyethylene terephthalate.

4. The optical mirror according to claim 1, characterized in that the film (22) is metallized.

5. An optical mirror according to claim 2, characterized in that the membrane (22) has a coating made of aluminium.

6. An optical mirror according to claim 1, characterized in that the membrane (22) has a thickness in the range of a few micrometers.

7. The optic of claim 1, wherein the recess is a circular hole.

8. The optical mirror according to claim 1, characterized in that the carrier (21) is embodied as a merely rectangular frame, onto which a mirrored film (22) is laid or attached.

9. An X-ray fluorescence analysis apparatus comprising an X-ray source (10) for irradiating a sample (15) with an X-ray beam (19); an X-ray detector (17) for measuring X-ray fluorescence radiation (16) emitted by the sample; and a camera (25) for producing an optically controlled image (26) of the irradiated position of the specimen (15) via an optical mirror (20) which is arranged angularly in the beam path of the X-ray source (10), the optical mirror comprising a carrier (21) on which a mirror layer (28) is provided, characterized in that the optical mirror (20) is an optical mirror formed in accordance with claim 1.

10. The X-ray fluorescence analysis device according to claim 9, characterized in that the camera (25) is implemented as an endoscope.

11. The X-ray fluorescence analysis device according to claim 9, characterized in that a single capillary lens or a multi-capillary lens is arranged before the optical mirror (20).

12. A method for X-ray fluorescence analysis of a sample (15) for determining the thickness of a thin layer, wherein the sample (15) is irradiated with a polychromatic X-ray beam (19) from an X-ray source (10), X-ray fluorescence radiation (16) emitted by the sample (15) is measured with an X-ray detector (17), an optically controlled image (26) of a measurement position (29) of the sample (15) is generated with a camera (25) via an optic (20) which is arranged angularly in the beam path of the X-ray source (10), the optic comprising a carrier (21) on which a mirror layer (28) is provided, characterized in that,

the optical mirror (20) is according to any one of claims 1 to 8 and is penetrated by an X-ray beam (13), wherein the X-ray beam (13) first enters and passes through a recess (23) of the carrier (21) and subsequently through the membrane (22), and an optical image is reflected by a measurement position (29) of the specimen (15) on the membrane (22) and the optical image is detected by the camera (25).

Technical Field

The invention relates to an optical mirror, in particular for an X-ray fluorescence analysis device; and to an X-ray fluorescence analysis apparatus, wherein the X-ray fluorescence analysis apparatus has an X-ray source for irradiating a sample with X-ray radiation, an X-ray detector for measuring the X-ray fluorescence radiation emitted by the sample, and a camera, wherein the camera produces an optical image of the irradiated position of the sample via an optical mirror arranged at an angle on the beam path of the X-ray source. Furthermore, the invention relates to a corresponding method for X-ray fluorescence analysis, in particular for determining the thickness of thin layers.

Background

X-ray fluorescence analysis is a non-destructive method for qualitative and quantitative material analysis. The method is based on the principle that by irradiating a sample with polychromatic X-ray radiation, electrons are released from the inner shells of the atoms forming the sample. The gaps between the atoms are filled with electrons from the inner shell. During these conversions, characteristic fluorescence radiation in the X-ray range occurs, which is recorded by the detector and provides information about the elemental composition of the sample.

X-ray fluorescence analysis is also particularly suitable for layer thickness measurement of thin layers and layer systems. Since the X-rays penetrate the lamellae, X-ray fluorescence radiation is also generated in the material situated below the lamellae, which X-ray fluorescence radiation is attenuated by absorption in the overlying layers on its way to the detector. Both the material composition and the current layer thickness can be determined by evaluating the spectrum in the wavelength range of the X-ray radiation. In order to achieve good spatial resolution, the measuring point, the so-called region of the specimen, which is detected by the primary radiation, has to be chosen comparatively small.

In the investigation of samples by means of X-ray fluorescence analysis, the measurement points have to be adjusted via an optical image of the sample surface. This is typically done using a video camera. However, in order to produce a parallax-free image of the measurement position of the sample, the control acquisition must be as parallel as possible to the X-ray beam/X-ray beam. For this purpose, the optical mirror is arranged in the beam path directed at an angle to the camera. However, in order for the mirror not to absorb the X-ray beam on its way to the measurement location, the mirror must have an aperture in the region of passage of the X-ray beam. Such an optical mirror is known from DE 3314281 a 1. However, a disadvantage of this optical mirror is that it must be fixed at a distance from the sample surface in order to produce an interference-free image.

An optical mirror with a hole for passing an X-ray beam is used for producing an X-ray fluorescence analysis device for controlled recording, as is known, for example, from DE 19710420 a 1. In EP 1348949B 1, focusing X-ray optics are additionally employed, which are guided through a recess in the control mirror. The same is known from DE 3239379C 2, which discloses a mirror in which the size of the aperture can be adjusted for the passage of the X-ray beam.

Furthermore, an X-ray fluorescence analysis apparatus and a method for X-ray fluorescence analysis are known from US 4,406,015 a, wherein a mirror is arranged in a main beam, said mirror having an evaporation deposited onto SiO₂An aluminum layer on a plate or an aluminum layer evaporated onto a plastic film. The mirror thus comprises a full-surface SiO or on a full-surface carrier formed from plastic₂An aluminum layer on the sheet.

A disadvantage of both embodiments is that these full-surface carriers reduce the intensity of the X-ray radiation directed at the measuring obj ect and thus require more measuring time. Additionally, an embodiment in which the carrier is made of plastic has the disadvantage that the plastic is eroded by the irradiation with X-ray radiation over the course of time.

Disclosure of Invention

The object of the invention is to improve an optical mirror, an X-ray fluorescence analysis device and a method for X-ray fluorescence analysis such that a natural control recording can be achieved at the measurement position of the sample to be analyzed, and this when the sample is located at a very short distance from the mirror.

The above-mentioned objects and advantageous embodiments result from the following.

According to one aspect of the present invention, an optical mirror for an X-ray fluorescence analysis apparatus is provided, wherein the X-ray fluorescence analysis apparatus has an X-ray source for irradiating a sample with an X-ray beam; an X-ray detector for measuring X-ray fluorescence radiation emitted by the sample; and a camera for producing an optically controlled image of the irradiated measurement location of the sample via the optical mirror, which is arranged angularly in the beam path of the X-ray source, which optical mirror comprises a carrier on which a mirror layer is arranged, wherein the carrier has a flat base body with a recess in the region of a through-window for the X-ray beam, and a film covering the flat base body and the recess forms the mirror layer on the outside of the carrier, wherein the film is bonded to the carrier and covers the recess of the carrier in a tensionless manner, and wherein the flat base body is made of glass.

Preferably, the membrane is made of plastic.

Preferably, the film is made of polyethylene terephthalate.

Preferably, the membrane is metallized.

Preferably, the membrane has a coating made of aluminium.

Preferably, the membrane has a thickness in the range of a few microns.

Preferably, the recess is a circular hole.

Preferably, the carrier is embodied as a merely rectangular frame, onto which the mirrored film is laid or attached.

According to another aspect of the present invention, there is provided an X-ray fluorescence analysis apparatus comprising: an X-ray source for irradiating a sample with an X-ray beam; an X-ray detector for measuring X-ray fluorescence radiation emitted by the sample; and a camera for producing an optically controlled image of the irradiated position of the sample via an optical mirror, the optical mirror being arranged angularly in the beam path of the X-ray source, the optical mirror comprising a carrier on which a mirror layer is provided, wherein the optical mirror is an optical mirror formed as described above.

Preferably, the camera is implemented as an endoscope.

Preferably, a single capillary lens or a multi-capillary lens is arranged before the optical lens.

According to a further aspect of the invention, there is provided a method for X-ray fluorescence analysis of a sample for determining the thickness of a thin layer, wherein the sample is irradiated with a polychromatic X-ray beam from an X-ray source, X-ray fluorescence radiation emitted by the sample is measured with an X-ray detector, an optically controlled image of the measurement position of the specimen is generated with a camera via an optical mirror which is arranged angularly in the beam path of the X-ray source, the optical mirror comprising a carrier on which a mirror layer is arranged, wherein the optical mirror is an optical mirror as described above and is penetrated by an X-ray beam, wherein the X-ray beam first enters and passes through the recess of the carrier and subsequently passes through the membrane, and an optical image is reflected by the measurement position of the specimen on the film, and the optical image is detected by the camera.

The object of the invention is achieved by an optical mirror having a through-window for X-ray radiation, wherein the through-window is formed by a recess in the carrier and a film covering the recess on the outside of the carrier, which film forms a mirror layer. Such an optical mirror is transparent on the one hand to X-rays, in particular the primary radiation of X-ray radiation, with high intensity, since only the membrane is transparent and not to optical radiation, in order to detect an image of the surface of the measurement site of the specimen, so that a complete image of the measurement site can be detected by the camera.

The micro-optics may be created by such an optical mirror, and thus the distance between the focal point on the sample and the X-ray optics may be kept low by maintaining the position of the optical mirror for direct viewing of the sample. Thus, a compact or space-saving construction of the X-ray fluorescence analysis apparatus is achieved.

Preferably, the film is made of plastic, particularly preferably polyethylene terephthalate. The plastic mainly comprises carbon with an atomic number of only 6. For the atomic number z of the material to be transmitted due to X-ray absorptionHas very strong dependence (about-z)⁴) The weakening caused by the plastic film is very low. A particularly tear-resistant film may be made of polyethylene terephthalate, PET for short, especially if such a film is biaxially stretched.

The film may be metallized in order to obtain a reflective coating on the film or to form a mirror layer. The metallization can be realized in a simple manner, for example, by means of sputtering (cathode atomization) or vacuum plating.

Preferably, a mirror coating made of aluminum is applied, since aluminum has the lowest atomic number of metals considered for mirroring and can also be sputtered very well.

Such a film applied to the carrier can be embodied particularly thin, for example with a thickness of only a few micrometers, so that the main X-ray beam is hardly attenuated, the absorption of which depends exponentially on the thickness of the material to be transmitted.

In order to be able to obtain a stable optical mirror, the carrier has a flat base body, preferably made of glass, with a recess, preferably a circular hole, in the region of the through-window. The mirrored film can be applied or bonded to a carrier, wherein the bonding points need only be provided, for example, in the edge region.

In particular, a stress-free arrangement of the film in the region of the recess of the carrier can be achieved by bonding the film to the carrier. The film is therefore only active in the region of the mirror that is transparent to light, which however hardly results in a loss of intensity of the X-ray beam.

Alternatively, the optical mirror can also have a frame as a carrier, onto which frame a mirrored film is laid or attached.

The object of the invention is also achieved by an X-ray fluorescence analysis device, wherein an optical mirror with a through window for the X-ray beam is used, said optical mirror comprising a carrier with a recess, said recess being covered by a film, said film forming a mirror layer on the outside of the carrier.

The optical image can thus be detected by the measuring position of the sample, which can be analyzed for measurement control.

The endoscope may be used as a video camera, for example a video endoscope. Due to the compact type of construction achieved in this way, a focusing X-ray optic is employed and is positioned very close to the specimen surface. A very good spatial resolution is thus obtained.

Preferably, a single or multi-capillary lens is positioned in front of the mirror, viewed in the direction of the beam, so as to focus the main beam and enable a smaller measurement shot on the measurement surface.

The object of the invention is also achieved by a method for X-ray fluorescence analysis of a sample, wherein the optical mirror comprises a carrier with a through-window for the X-ray beam, for example a through-hole or a recess, which is covered by a film on the outside of the carrier, which forms a mirror surface, such that only the film of the optical mirror is transmitted by the X-ray beam and a complete and deformation-free optical image is reflected by the measurement position of the sample on the film or the sample surface, which is formed as a mirror layer and which is detected by a camera.

Thus, an improved evaluation and monitoring of the measurement at the measurement location of the specimen may be achieved. Additionally, movement of the specimen between the X-ray beam and its adjacently positioned mirror is not necessary in order to detect a complete image of the measurement position of the specimen. This is because the optical mirror can be formed as a space-saving optics and can still be located between the X-ray beam and the measurement position during the measurement.

Drawings

The invention and further advantageous embodiments and modifications thereof are described and explained in more detail below with the aid of examples shown in the drawings. The features from the description and the drawings may be employed separately or together in any combination in accordance with the invention. In which is shown:

FIG. 1 is a schematic view of an X-ray fluorescence analysis apparatus having an optical mirror according to the present invention;

FIG. 2 is a perspective view of the optical lens of the first embodiment; and is

Fig. 3 is a perspective view of the optical mirror of the second embodiment.

Detailed Description

The X-ray fluorescence analysis apparatus 9 shown in fig. 1 includes an X-ray tube 10 of conventional construction having a hot cathode 12 as an X-ray source from which electrons are emitted and which utilizes an acceleration voltage U_BAnd is accelerated to collide with the anode 11. At the anode, the electrons are braked and an X-ray beam/X-beam 13 is generated. The wavelength range of the polychromatic X-ray beam 13 depends on the acceleration voltage U_BAcceleration voltage U_BTypically ranging from about 10kV, for example to 50kV in the illustrative embodiment, and the anode material is, for example, tungsten.

The X-ray beam 13 is then preferably focused by X-ray optics 14, which in the exemplary embodiment are formed by a mono/single capillary (monocapillary) or multi/multi-capillary (polycapillary) lens. Alternatively, only a simple collimator may also be used for blanking the beam 19.

The blanked or concentrated beam 19 then impacts the test specimen 15. The test specimen 15 comprises, for example, a layer 15a or a layer system. The radiation beam 19 penetrates at least partially through the layer 15a or through the upper layer 15a or the layer system of the test specimen 15. Within the irradiated region, an X-ray fluorescence beam 16 is generated, which is detected by an X-ray detector 17, such as a semiconductor detector. The material composition of the sample 15 and/or the layer thicknesses of the layer 15a or of the layer system can be determined by evaluating the measured energy spectrum 18 of the X-ray fluorescence beam 16 in a known manner.

At the same time, the X-ray fluorescence analysis apparatus allows direct video observation of the specimen surface at the measurement point 29. This serves for control and, for example, simplifies the positioning of the test specimen 15 relative to the measurement point. Furthermore, the optically controlled recording of the sampled region or of the measurement location 29 can thus be stored for each X-ray fluorescence measurement, so that the orientation of the measurement location 29 can then be perfectly understood.

In order to be able to produce a parallax-free control recording, an image of the measurement location 29 is captured in parallel with the X-ray beam 19. For this purpose, the optical mirror 20 is arranged angularly in the beam path. Imaging optics, such as a lens 24, display an image of the sample surface at the measurement location 29 onto a camera 25, such as a digital CCD camera. Preferably, an endoscopic camera is provided which has a small size and can be positioned at a short distance from the optical lens. The image of the camera 25 is displayed on a monitor 26 and can be stored and analyzed with the measurement data set.

In order to be able to attenuate the X-ray beam 13 as little as possible by the optical mirror 20, the optical mirror has a through-window 30 for the X-ray beam 13. This through window 30 is formed by a recess 23 in the carrier 21, which is covered on one side of the carrier 21 by a light-transmitting film 22 as a mirror layer 28. The outside of the film 27 is mirrored. The carrier 21 is arranged in an inclined manner with respect to the measuring position 29 with this mirrored outer side of the film 22, so that the X-ray beam 13 first enters and passes through the recess 23 of the carrier 21 and subsequently penetrates the film 22 or passes through the film 22. The carrier 21 preferably comprises glass.

The absorption of the X-ray beam has, on the one hand, an exponential dependence with respect to the thickness of the material to be penetrated and, on the other hand, a very strong dependence proportional to the fourth power of the atomic number Z of the material to be penetrated. Glass may actually be used as a carrier material for the mirror 20 (silicon has an atomic number of 14), but the X-ray beam 13 can pass through the recess 23 without obstruction.

The continuous film 22, which is preferably made of plastic, is located on the underside of the optical mirror 20 facing the camera 25. The plastic substantially comprises carbon, the atomic number of which is 6. Additionally, plastic films can be made particularly thin, in the range of a few microns in thickness, but are particularly durable and tear resistant. A preferred plastic for making the film 22 is polyethylene terephthalate, PET for short. In particular, biaxial polyester films made of PET known under the names Mylar, Melinex or Hostaphan are suitable for use according to the invention.

For the purpose of mirroring, the plastic film 22 is metallized, for example a mirrored metal coating is applied to the film by sputtering (cathode atomization) or vacuum plating. Aluminum (atom number 13) is particularly suitable as coating material because of the smallest possible atom number, which can still be sputtered particularly well.

Metallized PET films suitable for current applications have typical material thicknesses, for example, of less than 100 μm, and have a high level of tear resistance. The reflective metallization coating may have a thickness of less than 100 nm. Due to the extremely low material thickness and its low atomic number of the metallized film 22, the film is substantially transparent to the X-ray beam 13. It therefore also successfully creates a continuous optic 20 with a substantially transparent through window 30.

The membrane 22 may be bonded, laminated or laid onto the flat substrate of the carrier 21. The bonding points may be limited to the edge area of the carrier 21. In fig. 2, such a mirror 20 is shown, for example. The carrier 21 has a circular hole as a through window 30, through which the X-ray beam 13 can pass. The membrane 22 is laid on the outside of the carrier 21 and covers the holes 23.

As an alternative to a carrier 21 made of a glass plate with round holes, the carrier 21 can also be embodied as a merely rectangular frame, on which the film 22 is laid and attached. This embodiment with a frame 21 as a carrier is shown for example in fig. 3. An advantage of this embodiment is that a larger area can be used as the through-window 30, so that the X-ray optics can be moved to scan the measurement point 29 relative to the sample 15, instead of moving the sample 15 under the X-ray optics 14.

The distance between the X-ray optics 14 and the specimen 15 amounts to about 15mm in the exemplary embodiment. Larger distances are possible, but lead to a poorer focusing of the X-ray beam 13 and thus to a poorer spatial resolution of the X-ray fluorescence analysis apparatus 9. Video endoscopes are particularly suitable due to their small size, in which the imaging optics 24 and the digital camera 25 are integrated in the form of an endoscope.

The features described above are all important for the invention itself and can be combined with one another in any way.