Abstract:
A device for measuring the pulse transfer of X-ray quanta which are elastically scattered in an examination zone, includes an X-ray source which is arranged on one side of the examination zone, a detector which is situated on the other side of the examination zone and which measures the energy of the X-ray quanta, and a rotationally-symmetrical diaphragm device which is arranged between the detector and the X-ray source. In a device of this kind a comparatively accurate determination of the pulse transfer is also possible for thick objects, because the diaphragm device is constructed so that the X-ray quanta emitted by the X-ray beam source are transmitted to the examination zone only on the envelope of a cone.
Abstract:
The invention relates to a method of determining the share of different chemical elements in a layer of an examination zone. The Compton scattered radiation and the Rayleigh scattered radiation are separately determined and the variation of the differential scatter coefficients derived from the measurement values is influenced by the shares of the various chemical elements contained in the individual pixels. Therefore, the share of these chemical elements can be determined therefrom.
Abstract:
The invention relates to a device for examining a body by means of gamma rays or X-rays, in which a body to be examined is irradiated by a plurality of primary beams having a comparatively small cross-section. The scattered radiation produced is intercepted by detector devices, at least one of which is associated each time with a respective primary beam, and the detector device and an associated slit which images the primary beam on the detector device is arranged so that the detector device is struck essentially only by scattered radiation from this one primary beam. Preferably, the detectors are arranged between the body to be examined and the radiation source, so that they can intercept only the back-scattered radiation.
Abstract:
A scatter radiation device for determining the internal structure of a body comprises a monoenergic radiation source for emitting a narrow primary beam which penetrates the body, at least one slit diaphragm device which is situated outside the primary beam and which comprises a plurality of slit diaphragm apertures which extend approximately perpendicularly to the primary beam, and a detector device which extends transversely of the longitudinal slit direction and which comprises separate detectors which receive scatter radiation produced in the body by the primary beam. The scatter radiation which each time originates from a point of the primary beam and which passes through all slit diaphragm apertures, is measured by different detectors of the detector device, and thus serves for determining the body density at the corresponding point.
Abstract:
A method for making a secondary collimator that includes at least one plate having a plurality of slits defined therein includes determining a gap thickness between plate positions of the secondary collimator based on at least one dimension of the at least one plate and fabricating a base plate from a base plate blank. The base plate includes at least two slots being spaced apart by the gap thickness. The at least one plate is inserted into a first slot of the at least two slots to form the secondary collimator.
Abstract:
An integrated, multi-sensor, Level 1 screening device is described, which system provides a next-generation Explosives Detection System (EDS) that enables high throughput, while drastically reducing false alarms. In exemplary embodiments, the present system comprises a non-rotational, Computed Tomography (CT) system and a non-translational, X-ray diffraction (XRD) system, both in an inline configuration.
Abstract:
A method for operating an X-ray diffraction imaging (XDI) system to scan an object includes generating an X-ray beam from at least one source focus at a first focus location, and receiving first scatter radiation at a first scatter angle at a scatter detector. The first scatter radiation is produced when the X-ray beam interacts with the object. The method further includes displacing the at least one source focus from the first focus location to a second focus location, generating a displaced X-ray beam from the at least one source focus at the second focus location, and receiving second scatter radiation at a second scatter angle at the scatter detector. The second scatter radiation is produced when the displaced X-ray beam interacts with the object. An identification of the object based on one of the first scatter radiation and the second scatter radiation is output.
Abstract:
A method to account for cross-talk among a plurality of coherent scatter detectors of a multi-detector inverse fan beam x-ray diffraction imaging (MD-IFB XDI) system. The MD-IFB XDI system includes a multi-focus x-ray source (MFXS) that emits radiation sequentially from a plurality of focus points denoted by F1, F2, . . . Fn with a running index i. The method includes measuring a diffraction profile Xk for each coherent scatter detector Dk of the plurality of coherent scatter detectors. The diffraction profile includes a spectrum of a number of photons measured in a plurality of corresponding coherent scatter detectors. Each coherent scatter detector Dk is corrected to remove scatter from a plurality of primary beams directed to remaining coherent scatter detectors of the plurality of coherent scatter detectors.
Abstract:
System and method for XRD-based false alarm resolution in computed tomography (“CT”) threat detection systems. Following a scan of an object with a megavoltage CT-based threat detection system, a suspicious area in the object is identified. The three dimensional position of the suspicious area is used to determine a ray path for the XRD-based threat detection system that provides minimal X-ray attenuation. The object is then positioned for XRD scanning of the suspicious area along this determined ray path. The XRD-based threat detection system is configured to detect high density metals (“HDMs) as well as shielded Special Nuclear Materials (“SNMs”) based on cubic or non-cubic diffraction profiles.
Abstract:
A system and methods for characterizing an unknown substance is described. One of the methods include determining an effective atomic number of the unknown substance as a first function of a first gradient of a first line.