G01N2223/501

RADIATION PHASE-CONTRAST IMAGING DEVICE

Provided is a radiation phase-contrast imaging device capable of assuredly detecting a self-image and precisely imaging the internal structure of an object. According to the configuration of the present invention, the longitudinal direction of a detection surface of a flat panel detector is inclined with respect to the extending direction of an absorber in a phase grating. This causes variations in the position (phase) of a projected stripe pattern of a self-image at different positions on the detection surface. This is therefore expected to produce the same effects as those obtainable when a plurality of self-images are obtained by performing imaging a plurality of times in such a manner that the position of the projected self-images on the detection surface varies. This alone, however, results in a single self-image phase for a specific region of the object. Therefore, according to the present invention, it is configured such that imaging is performed while changing the relative position of the imaging system and the object.

TWO-DIMENSIONAL X-RAY DETECTOR POSITION CALIBRATION AND CORRECTION WITH DIFFRACTION PATTERN
20170343490 · 2017-11-30 ·

A method of determining the spatial orientation of a two-dimensional detector in an X-ray diffractometry system, and calibrating the detector position in response thereto, uses diffraction patterns from a powder sample collected at a plurality of detector swing angles. The overlapping of the detected patterns indicates relative errors in the detector orientation. In particular, intersection points between the different diffraction patterns may be located, and their relative locations may be used to identify errors. Such errors may be in the detector position, or they may be errors in different rotational directions, such as roll, pitch or yaw. Determination and correction of the detector orientation using this method may be part of a calibration routine for the diffractometry system. Roll error may also be determined using a single measurement with the detector at a swing angle perpendicular to the X-ray beam.

DEVICE FOR SORTING MATERIALS, IN PARTICULAR SCRAP PARTICLES, BY MEANS OF X-RAY FLUORESCENCE
20170328845 · 2017-11-16 ·

A device for identifying materials on a conveyor belt (101) by means of X-ray fluorescence comprising an X-ray source (102), from which X-ray radiation (103) is guided onto material parts (104), comprising a detector head (107) containing an X-ray detector array (108) having a multiplicity of detector elements (113, 114, 115) arranged in a planar fashion for receiving X-ray radiation (105) and for converting said X-ray radiation into electrical charge signals, and also an electronic unit (109) for reading out and processing the charge signals, which comprises for each individual detector element a signal channel (120) having in each case: a discriminator unit (117) having at least two adjustable discriminator thresholds (116, 122) for detecting all Gaussian curve-like signals (119) whose amplitude is greater than one of the two or simultaneously greater than both discriminator thresholds, and also one counting unit (118, 121) per discriminator threshold for converting the signals into digital counting events,
wherein the individual detector elements of the X-ray detector array have a spatial resolution of 50 μm to 500 μm with a sensitivity to X-ray radiation in an energy range of between 500 eV and 30 keV, with an energy resolution of less than 0.5 keV at counting rates of up to 100 kcps and relative to an energy of 8.04 keV, the electronic unit comprises a signal channel for each individual detector element of the X-ray detector array,
and each discriminator unit for a specific detector element is in each case electrically connected to the discriminator units of the detector elements that are spatially directly adjacent to said detector element, wherein all the discriminator units are interconnected with one another via a digital and/or analog circuit in such a way that simultaneous occurrence of signals on more than one detector element can be identified and treated electrically separately.

METHOD AND SYSTEM FOR INSPECTING A STRUCTURE ACROSS A COVER LAYER COVERING THE STRUCTURE
20230184701 · 2023-06-15 ·

There is described a method for inspecting a structure across a cover layer covering the structure. The method generally has emitting a high energy photon beam along a photon path extending across said cover layer and leading to a target point within said structure, resulting in scattering along at least first and second scatter paths originating from said target point and extending across said cover layer and away therefrom, said first and second scatter paths forming a respective angle relative to said cover layer and defining an inspection plane comprising at least the target point; simultaneously detecting a first scatter signal incoming from said first scatter path and detecting a second scatter signal incoming from said second scatter path, and generating first and second values indicative therefrom; comparing said first and second values to one another; and inspecting said structure based on said comparing.

BIOSENSOR

According to one embodiment, a biosensor includes a substrate and a sensor matrix that is present in a two-dimensional region on the substrate. The sensor matrix includes a plurality of basic blocks. Each of the basic blocks includes at least three types of sensor elements.

INDIRECT CONVERSION DETECTOR ARRAY
20170248705 · 2017-08-31 ·

Among other things, a detector array (300) for a radiation imaging system is provided. The detector array comprises a plurality of detector elements. Respective detector elements comprise, among other things, a scintillator (304) and a photodetector (306). In some embodiments, a scintillator is shared amongst two or more of the detector elements. In some embodiments, little to no reflective material, configured to mitigate cross-talk between detector elements, is situated between two or more detector elements.

System and method for material characterization

The invention provides a system and method for characterising at least part of a material comprising: a source of incident X-rays (4, 28) configured to irradiate at least part of the material; one or more detectors (300,302,312,1701,1704,1600,1607,1608,1604) adapted to detect radiation emanating from within or passing through the material as a result of the irradiation by the incident radiation (1700) and thereby produce a detection signal (313); and one or more digital processors (304-311,2000-2009) configured to process the detection signal (313) to characterise at least part of the material; wherein the one or more detectors (300,302,312,1701, 1704,1600,1607,1608,1604) and one or more digital processors (304-311,2000-2009) are configured to characterise at least part of the material by performing energy resolved photon counting X-ray transmission spectroscopy analysis.

METHODS FOR 2-COLOR RADIOGRAPHY WITH LASER-COMPTON X-RAY SOURCES
20170241920 · 2017-08-24 ·

High-contrast, subtraction, x-ray images of an object are produced via scanned illumination by a laser-Compton x-ray source. The spectral-angle correlation of the laser-Compton scattering process and a specially designed aperture and/or detector are utilized to produce/record a narrow beam of x-rays whose spectral content consists of an on-axis region of high-energy x-rays surrounded by a region of slightly lower-energy x-rays. The end point energy of the laser-Compton source is set so that the high-energy x-ray region contains photons that are above the k-shell absorption edge (k-edge) of a specific contrast agent or specific material within the object to be imaged while the outer region consists of photons whose energy is below the k-edge of the same contrast agent or specific material. Scanning the illumination and of the object by this beam will simultaneously record and map the above edge and below k-edge absorption response of the object.

MEASUREMENT ARRANGEMENT FOR X-RAY RADIATION FOR GAP-FREE ID MEASUREMENT

In summary, the present invention proposes embodying an X-ray detector (21) with a plurality of detector modules (1, 1a-1g), each comprising dead zones (6) without X-ray sensitivity and active zones (3, 3a-3c) with X-ray sensitivity that is spatially resolved in a measurement direction (MR), wherein the detector modules (1, 1a-1g) are embodied successively and in an overlapping fashion along the measurement direction (MR), such that in overlap regions (23a-23e) the dead zone (6) of one detector module (1, 1a-1g) is bridged by an active zone (3, 3a-3c) of another detector module (1, 1a-1g). The overlapping detector modules (1, 1a-1g) are arranged next to one another in the transverse direction (QR) in the overlap regions (23a-23e), wherein the transverse direction (QR) runs transversely with respect to the local measurement direction (MR) and transversely with respect to a local connection direction (VR) with respect to a sample position (91). The X-ray detector (21) makes it possible, in a simple manner, to obtain gapless, one-dimensional measurement information, in particular X-ray diffraction information, from a measurement sample (96) at the sample position (91).

Method for establishing a spectral response function of a system for measuring with X-rays or gamma rays

A method for determining a response of a spectrometric system for measuring ionizing x-ray or gamma-ray photons, the measuring system comprising: a radiation source, configured to emit ionizing radiation along an emission axis; a pixelated detector, which comprises pixels, each pixel being configured to detect radiation emitted by the radiation source, and to acquire thereof an energy spectrum, in a plurality of energy channels; the emission axis being an axis extending between the radiation source and the detector;
the response of the measuring system taking the form of effective spectra, defined for each pixel, and in each energy band, the effective spectrum of a pixel, in an energy band, corresponding to an energy distribution of the photons detected, by the pixel, in the energy channel, in the absence of any object interposed between the source and the pixel.