Patent classifications
G01N2223/50
SYSTEM AND METHOD FOR ELECTRON CRYOMICROSCOPY
A system and corresponding method for electron cryomicroscopy, comprising: a field-emission gun for generating an electron beam, the field-emission gun being energized, in use, to generate a 80 keV to 120 keV electron beam which is emitted into a vacuum enclosure and towards a specimen holder; the vacuum enclosure containing, at least in part: an objective lens for focusing an image of the specimen, the objective lens being disposed in the path of the electron beam and having a chromatic aberration coefficient, Cc, selected to achieve a resolution value better than a desired amount; the specimen holder for holding a specimen, the specimen holder being disposed in the path of the electron beam; a cryostage for cooling a specimen; a cryo-shield for surrounding a specimen and reducing an ice contamination rate of the specimen; and a direct electron detector comprising an array of pixels, each pixel capable of detecting an incident electron that has passed through a sample and struck the pixel.
X-RAY INSPECTION APPARATUS, X-RAY INSPECTION SYSTEM, AND X-RAY INSPECTION METHOD
An X-ray inspection apparatus includes a transport unit configured to transport an article, an electromagnetic wave irradiation unit configured to irradiate the article with a first electromagnetic wave in a first energy band and a second electromagnetic wave in a second energy band, an electromagnetic wave sensor configured to detect the first electromagnetic wave and the second electromagnetic wave, and a control unit to which a detection result is input. The control unit is configured to generate a first transmission image based on a detection result of the first electromagnetic wave and a second transmission image based on a detection result of the second electromagnetic wave, to perform image processing including a subtraction process on the first transmission image and the second transmission image, and to determine whether or not a foreign material is included in the article on the basis of a difference image.
AN ENERGY DISPERSIVE X-RAY DIFFRACTION ANALYSER HAVING AN IMPROVED REFLECTION GEOMETRY
An on-line energy dispersive X-ray diffraction (EDXRD) analyser for mineralogical analysis of material in a process stream or a sample is disclosed. The analyser includes a collimated X-ray source to produce a diverging beam of polychromatic X-rays, and an energy resolving X-ray detector, and a substantially X-ray transparent member having the form of a solid of revolution which is circularly symmetric about a central axis between the collimated X-ray source and the energy resolving X-ray detector, an outer surface of the X-ray transparent member positionable adjacent the material to be analysed. A primary beam collimator is disposed adjacent to or within the substantially X-ray transparent member to substantially prevent direct transmission of polychromatic X-rays emitted from the source to the detector. The analyser is configured such that the diverging beam of polychromatic X-rays are directed towards the substantially X-ray transparent member, and where the energy resolving X-ray detector collects a portion of the beam of X-rays diffracted by the material and outputs a signal containing energy information of the collected, diffracted X-rays.
X-RAY DETECTOR AND DRIVING METHOD THEREFOR
Disclosed is an x-ray detector includes a first electrode formed on a substrate, a photoconductive layer formed on the first electrode, a second electrode formed on the photoconductive layer and configured to be in a voltage applied state with a bias voltage or a floating state, and a power supply circuit configured to control an output of the bias voltage to be on/off.
Multi-modal Compton and single photon emission computed tomography medical imaging system
A multi-modality imaging system allows for selectable photoelectric effect and/or Compton effect detection. The camera or detector is a module with a catcher detector. Depending on the use or design, a scatter detector and/or a coded physical aperture are positioned in front of the catcher detector relative to the patient space. For low energies, emissions passing through the scatter detector continue through the coded aperture to be detected by the catcher detector using the photoelectric effect. Alternatively, the scatter detector is not provided. For higher energies, some emissions scatter at the scatter detector, and resulting emissions from the scattering pass by or through the coded aperture to be detected at the catcher detector for detection using the Compton effect. Alternatively, the coded aperture is not provided. The same module may be used to detect using both the photoelectric and Compton effects where both the scatter detector and coded aperture are provided with the catcher detector. Multiple modules may be positioned together to form a larger camera, or a module is used alone. By using modules, any number of modules may be used to fit with a multi-modality imaging system. One or more such modules may be added to another imaging system (e.g., CT or MR) for a multi-modality imaging system.
Two-step material decomposition calibration method for a full size photon counting computed tomography system
A method and a system for providing calibration for a photon counting detector forward model for material decomposition. The flux independent weighted bin response function is estimated using the expectation maximization method, and then used to estimate the pileup correction terms at each tube voltage setting for each detector pixel.
TWO-STEP MATERIAL DECOMPOSITION CALIBRATION METHOD FOR A FULL SIZE PHOTON COUNTING COMPUTED TOMOGRAPHY SYSTEM
A method and a system for providing calibration for a photon counting detector forward model for material decomposition. The flux independent weighted bin response function is estimated using the expectation maximization method, and then used to estimate the pileup correction terms at each tube voltage setting for each detector pixel.
DIGITAL ENCODING ALGORITHM FOR PIXELATED DETECTORS
A detector for imaging and efficiently digitizing a spatial distribution of photon flux includes pixel circuits that compressively encode pixel values generated by integrated analog to digital converters (ADCs). On-pixel digital compression circuits (DCCs) implement compression to increase continuous frame rate by reducing the number of bits per pixel while keeping quantization error below Poisson noise. Several mapping algorithms for photon-counting and charge-integrating detectors and compact digital logic implementations are presented.
X-Ray Detection Apparatus and Method
A mask member is provided at an entrance opening of a mirror unit. Of a first diffraction grating and a second diffraction grating, when the second diffraction grating is used, the mask member masks preceding mirrors. With this process, aberration caused by reflective X-ray is suppressed. When the first diffraction grating is used, the mask member does not function. Alternatively, the mask member and another mask member may be selectively used.
TRANSMISSION X-RAY DIFFRACTION APPARATUS AND RELATED METHOD
There is provided a transmission X-ray diffraction (XRD) apparatus, the transmission XRD apparatus including an X-ray source for generating a direct X-ray beam; sample holder for receiving the sample, the sample being positioned to receive the direct X-ray beam when held by the sample holder; a detector for receiving X-rays transmitted through the sample and outputting an X-ray diffraction pattern therefrom; and an optical element positioned between the X-ray source and the detector, the optical element including a Montel optic and a secondary pin-hole collimator collectively adapted to focus the direct X-ray beam on the detector, wherein a ratio between a dimension of the direct X-ray beam projected on the detector and a sample-to-detector distance is equal or smaller than 1/570. Related methods are also provided.