Abstract:
The invention describes a method of generating metabolic images of an investigation region (3) of a body (1) by irradiating an X-ray fluorescence marker in that region and detecting the resulting X-ray fluorescence with a fluorescence detector (30). A fan beam (12) is used as a source of primary X-radiation, thus allowing the scanning of a whole body slice (3) in one step. The fluorescence image may be directly measured, e.g. by mapping voxels (104) of the investigation region onto pixels (134) of the detector (130) with the help of a pinhole collimator (132), or it may be reconstructed by procedures of computed tomography. Moreover, a morphological image may be generated by simultaneously recording X-ray transmission through the body (1).
Abstract:
An imaging system for generating a diffraction profile is described. The imaging system includes a gantry including an x-ray imaging system configured to generate an x-ray image of a substance and a scatter system configured to generate a diffraction profile of the substance.
Abstract:
An examination apparatus, such as for inspection of baggage or any object of interest, has a source of radiation which is moved during scanning of the object of interest. A scattered radiation are detected which is scattered by the object of interest under a particular predetermined scatter angle, without moving the detector array. By detecting the scatter radiation scattered under the predetermined scatter angle, the vertical coordinate of the location of the scatter center in the object of interest and its composition may be derived.
Abstract:
The present invention relates to an X-ray source comprising an electron source (1) for the emission of electrons (E), a target (4) for the emission of characteristic, substantially monochromatic X-rays (C) in response to the incidence of the electrons (E) and an outcoupling means (11) for outcoupling of the X-rays. To achieve characteristic, substantially monochromatic X-rays with a high power loadability electrons are incident on a metal foil (5) of a thickness of less than 10 μm and a base arrangement (7, 12) is arranged wherein the metal of said metal foil (5) has a high atomic number allowing the generation of X-rays (C) and the material substantially included in the base arrangement (7, 12) has a low atomic number not allowing the generation of X-rays (C). The outcoupling means are adapted for outcoupling only X-rays (C) on the side of the metal foil (5) on which the electrons (E) are incident and which is opposite to the side of the base arrangement (7, 12) since on this side almost no bremsstrahlung radiation is generated.
Abstract:
The invention relates to a method and a device for determining the distribution of an X-ray fluorescence (XRF) marker (16) in a body volume (14). The body volume (14) is irradiated with a beam of rays (12) from an X-ray source (10) with a first ray component with a quantum energy just above and a second ray component with a quantum energy just below the K-edge of the XRF marker (16). Secondary radiation emitted from the body volume (14) is detected in a location-resolved way by a detector (30). To separate the X-ray fluorescence components in the secondary radiation from background radiation, the body volume is irradiated for a second time with a beam of rays from which the first ray component has been substantially removed by a filter (22) made from the material of the XRF marker.
Abstract:
A method for classifying an unknown substance is provided, The method includes classifying the unknown substance based on simultaneously processing a plurality of parameters determined from a plurality of signals that are measured by at least one detector. The at least one detector is located within a gantry of an imaging system.
Abstract:
A method for reducing an artifact within an image of a substance is described. The method includes generating the image of the substance, and constraining a measured linear attenuation coefficient of a pixel of the image based on at least one of a measured diffraction profile, a measured effective atomic number, and a measured packing fraction of the substance.
Abstract:
The invention relates to an electron window 1 for a liquid-metal anode 2 in the form of a membrane 4. It is provided according to the invention that the electron window 1 has ridges 10 and depressions 11. In addition, the invention relates to a liquid-metal anode 2 into which such an electron window 1 according to the invention is inserted. The invention further relates to an X-radiator which has a liquid-metal anode 2 according to the invention. The invention also relates to a method for operating a liquid-metal anode 2 in which, during the production of X-radiation, stronger turbulence 5 is produced in the flow of the liquid metal below the electron window 1 at the ridges 10.
Abstract:
Examination apparatus for baggage inspection are usually bulky and comprise mechanical components requiring precision movements. According to the present invention, examination of an object of interest is provided by moving a source of radiation (1) during scanning of the object of interest (11) and detecting a transmitted beam of radiation (4) and a scattered radiation (3), which is scattered by the object of interest (11) under a particular predetermined scatter angle, without moving the detector array (5,6). Advantageously, by detecting the scatter radiation scattered under the predetermined scatter angle, the vertical coordinate of the location of the scatter center in the object of interest and it's composition may easily be derived.
Abstract:
The invention relates to a system for measuring the pulse transmission spectrum of X-ray quanta that are elastically scattered in an examination zone for containers according to the preamble of claim 1. Corresponding systems that are based on the principle of examination with coherent scattered radiation are known from the prior art and from our previous application EP 11 06 227. These systems are problematic in that the electronic system required for controlling the X-ray capacity of the different focal points is too complicated and the measuring time is relatively long as only one focus is active at a time. This results in a low detection efficiency as the voxel geometry allows for non-scanned areas so that objects looked for in the container can be overlooked. The invention is based on the surprising finding that these problems can be overcome when the detector arrangement (D) has a two-dimensional segmenting in the Y, Z plane and lies before the Z axis and that the X-ray emitter (Q) is disposed with an elongated anode that emits radiation across its surface either completely or partially at the same time. The secondary antiscatter grid (S) runs in the Y direction converging to O and in the Z direction about the angle θ to the X axis in such a manner that Y and X of the scattered voxel in the container are coded onto the Y and Z dimensions of the detector arrangement (D) and that the primary antiscatter grid (P) and the X-ray emitter (Q) run in a cylindrically symmetrical orientation about the Z axis or in a linear/parallel orientation to the Y axis in the X,Y plane.