The invention relates to an X-ray source having a housing in which a target is provided which can emit X-rays when being bombarded with an electron beam. The invention additionally relates to a method for producing X-rays, in which a target in a housing of an X-ray source is bombarded with an electron beam. The invention finally also relates to the use of an X-ray source emitting monochromatic X-rays.
An X-ray source, the use thereof and a method for producing X-rays of the type mentioned in the introduction are disclosed, for example, in US 2008/0144774 A1. According to said document, an X-ray source can be realized by way of example by arranging electrodes within a housing. In the housing, an electron beam is produced by an electrode having a potential of 0 V. An anode, which is used as a target for the electron radiation, is arranged opposite said electrode. Said anode is at 100 kV. Located downstream of the anode is furthermore a collector which is at a potential of 10 kV. When the electron beam strikes the anode, X-rays are released which can be coupled out of the housing through a suitable window (transparent to X-rays) and be supplied for use.
The anode serving as a target can be configured as a thin-walled structure. By way of example, the anode may have a base plate made of boron, having a thickness of between 10 and 200 μm. A thin layer of tungsten having a layer thickness of 0.1 to 5 μm, which is used as a target, is applied on said base plate. However, the very thin tungsten layer is exposed to a high degree of stress on account of the electron beam.
In addition, according to DE 103 42 239 A1, an apparatus for producing soft X-rays, for example, with an electrically driven discharge is described. In this case, a laser beam is used to vaporize a supplied medium. The medium used can be, for example, a metal melt applied on the external surface of two electrodes. A plasma is ignited in the vapor using the electrodes, and the X-rays are coupled out.
It is an object of the invention to improve the X-ray source mentioned in the introduction such that a relatively long operating time of the X-ray source is possible without the target needing to be replaced. It is furthermore an object of the invention to specify a method for operating said X-ray source. Finally, it is an object of the invention to find a use for such an X-ray source.
This object is achieved according to the invention in that a plasma acting as an anode can be produced in the housing in the form of an ionized metal vapor as the target, wherein a target material and a vaporizer apparatus for producing the metal vapor are provided in the housing. The target material may be solid or liquid. It is vaporized by the vaporizer apparatus such that a metal vapor is produced in the housing. In the metal vapor, which can be exposed to a high voltage in the housing, X-rays can be produced through bombardment with an electron beam.
The object is furthermore also achieved by the method for producing X-rays indicated in the introduction, wherein a metal vapor is produced as a target in a vaporizer apparatus, wherein a target material is provided for producing the metal vapor. How this method works has already been described above.
Finally, the object is also achieved by the use of an X-ray source as claimed in one of claims 1 to 8, which emits monochromatic X-rays, for X-raying a body which forms differentiable contrasts at the wavelength of the X-rays used. The body may be a mechanical body, such as for example a component connection that is to be examined for defects in the connection. Another possibility is to examine a human or animal body. In any case, the wavelength of the monochromatic X-rays must be selected suitably so that contrasts form. The use of monochromatic X-rays as compared to X-rays having a wavelength spectrum has the advantage that sharper images can be produced, which allow more detailed statements regarding the examined object to be made.
According to an advantageous embodiment of the invention, provision is made for the housing to have a vaporization chamber for a metal to be vaporized, which vaporization chamber is connected via an opening, preferably a nozzle, to a residual volume of the housing. This construction has the advantage that the metal vapor can be metered relatively accurately via the nozzle. It is also possible to influence the shape of the cloud, for example by way of the nozzle form. Finally, the vaporization chamber is advantageously separated from the residual volume of the housing. This facilitates cleaning measures, for example, which become necessary in parts of the housing owing to the fact that the metal vapor can deposit itself on the chamber walls.
According to another embodiment of the invention, provision is made for an electrode to be provided as the vaporizer apparatus for igniting an arc between the electrode and the target material. This vaporizer apparatus is located in the housing, in which the resulting metal vapor is also intended to be excited by the electron beam to emit X-rays. An advantage that should be mentioned here is that such a housing unit is simple in terms of construction. For example, if soiling occurs on account of the deposition of metal vapor, said housing unit can simply be replaced.
In the simplest case, it is also sufficient to use a simple electrode as the electron emitter. The target in plasma form is excited by a high-current discharge originating from the electrode.
It is an advantage that a window is arranged in the wall of the housing, which window is transparent for the X-rays to be produced. The resulting X-rays can advantageously be coupled out of the housing through said window and be supplied for a planned use.
According to one advantageous embodiment of the invention, provision is made for the metal vapor to consist of a light metal or a plurality of light metals, preferably aluminum. Light metals within the context of the application are meant to designate metals and the alloys thereof, the density of which is below 5 g/cm3. Specifically, said definition applies to the following light metals: all alkali metals, all alkaline earth metals except for radium, in addition scandium, yttrium, titanium and aluminum. Further advantageous material groups for forming the metal vapor are tungsten, molybdenum and the group of the lanthanides. When selecting the target material, the emission spectrum of the K-shell is crucial. This is advantageously adapted using the application. Specifically, this is the element lanthanum and the 14 elements following lanthanum in the periodic table.
The use of metal vapor also has the advantage that, due to the excitation of the target using the electron beam, monochromatic X-rays can advantageously be produced. These are X-rays having only one wavelength, which has the advantage that X-radiographs can be imaged more sharply with monochromatic X-rays, for example. It is therefore also an alternative way of achieving the invention to use said monochromatic X-rays for X-raying a body, which body must be of a nature such that, at the wavelength of the used monochromatic X-rays, contrasts of the body appear on the image. The body may be a mechanical structure (mechanical or inanimate body), such as for example a component connection that is to be examined for inflow of air. Another possibility is to record X-radiographs of a human or animal body.
Further details of the invention will be described below with reference to the drawing. Identical or mutually corresponding drawing elements in the individual figures in each case have the same reference sign and are only explained again if there are differences between the individual figures. In the figures:
Illustrated in
In order to produce an electron beam 23, an electron gun 24 is provided, wherein the electron beam 23 passes into the housing 11. The electron beam interacts with the gaseous target and is electrostatically decelerated and collected by a collector 28. Finally, a window 29 is provided, through which the X-rays 21 which are produced can be coupled out of the housing 11.
The electron gun 24 has a cathode 30, which is at a potential of 0 V. It emits the electron beam 23, which is, focused by a lens 31, coupled out of the electron gun. The driving force here is a potential which is established by the ionized, gaseous target to be made to have a potential of +100 to +300 kV. The collector 28 is at a potential of between +40 and +120 kV.
However, the X-ray beam 21 is produced in the same way as described in
The electron emitter used is, according to
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2012/061479 | 6/15/2012 | WO | 00 | 12/12/2014 |