Abstract:
A material analyzer for identifying quantities of one or more elements in a material has a container for holding a material to be analyzed, a resonant gamma ray source unit for directing resonant gamma rays into the material in the container, and at least one detector for detecting gamma rays resonantly scattered by at least one predetermined element in the material. The resonant gamma ray source unit has an outer housing of gamma ray shield and neutron shield material, with an inner chamber and an aperture directed towards the container, a moving gamma ray generator source of a predetermined material mounted in the chamber, the material being selected from a predetermined group of materials which emit resonant gamma rays when exposed to neutrons, the source being directed towards said aperture, and a neutron source positioned in the chamber adjacent the gamma ray generator source.
Abstract:
As described in the methods of the present invention, x-ray photons derived from a microscopic solid-density plasma that is produced by optically focusing a high power laser beam upon a high atomic number target, may be use for phase-contast medical microimaging and also for absorptive microradiography. As described in the methods of the present invention, x-rays derived from a microscopic solid-density plasma are utilized as object illumination sources that are microscopic in at least one direction (so that ultrathin slicebeams and fan-beams are allowed, as are linear arrays of numerous clusterd parallel microbeams). Collimating optical devices of prior art are required.
Abstract:
A small angle x-ray diffraction scattering system has a vertical orientation, allowing for simplified analysis of liquid samples. The system may function in a beam-up or a beam-down configuration. An x-ray source provides an initial x-ray beam that is directed vertically along a primary beampath to a sample located on a sample support. The small angle scattered x-ray energy travels through a secondary beampath to a detector. The primary and secondary beampaths may be evacuated and separated from a sample chamber by fluid seals. Beam conditioning optics and a collimator may be used in the primary beampath, and a beamstop used in the secondary beampath. The sample chamber may have a microscope or camera, which may be movable, for observing the sample, and a translation stage for moving the sample in at least two dimensions.
Abstract:
A phase information restoring method improves estimation accuracy of phase by using radiation with energy of high transmittance when constructing a radiation image of a living organism such as a human body by the phase-contrast method. The phase information restoring method includes the steps of: (a) obtaining plural sets of detection data respectively representing plural kinds of radiation image information on a detection plane at a predetermined distance from an object by using plural radiations having different wavelengths with energy from 16 keV to 30 keV to detect intensity of the plural radiations transmitted through the object on the detection plane; and (b) restoring phase information on the radiations transmitted through the object on the basis of the plural sets of detection data so as to obtain phase data.
Abstract:
Disclosed herein is a method of evaluating the performance of an ion-exchange film. In the method, small-angle scattering curves for the ion-exchange film are obtained by an X-ray measuring apparatus that can detect X-rays scattered at small angles with respect to the axis of an X-ray applied to film. From the positions of the peaks on the small-angle scattering curves and the X-ray intensities at these peaks, the molecular structure of the ion-exchange film is determined, thereby to evaluate the performance of the ion-exchange film.
Abstract:
In the calibration and alignment of an X-ray reflectometry (nullXRRnull) system for measuring thin films, an approach is presented for accurately determining C0 for each sample placement and for finding the incident X-ray intensity corresponding to each pixel of a detector array and thus permitting an amplitude calibration of the reflectometer system. Another approach involves aligning an angle-resolved X-ray reflectometer using a focusing optic, such as a Johansson crystal. Another approach relates to validating the focusing optic. Another approach relates to the alignment of the focusing optic with the X-ray source. Another approach concerns the correction of measurements errors caused by the tilt or slope of the sample. Yet another approach concerns the calibration of the vertical position of the sample.
Abstract:
Certain embodiments include a system and method for scatter measurement and correction. The method includes performing a calibration scan using a phantom to measure a scatter signal ratio between scatter x-rays impacting a first detector ring and scatter x-rays impacting a second detector ring. The scatter signal ratio is used to determine a scatter scale factor. The method further includes positioning a collimator such that the first detector ring is occluded from a path of primary x-rays generated by a target. The method also includes executing a low exposure scan to obtain x-ray scatter data using the first detector ring and the second detector ring and applying the scatter scale factor to the scatter data to produce scaled scatter data. The method further includes obtaining image data using the first detector ring and/or the said second detector ring and adjusting the image data using the scaled scatter data.
Abstract:
A baggage inspection device based on coherent x-ray scatter has an x-ray source on one side of the scanning area and detectors on the other side of the scanning area. The detectors measure the energy of the scattered x-ray quanta. A primary ray collimator is arranged between scanning area and x-ray source. A secondary ray collimator for scattered rays is arranged between scanning area and detectors. The detectors are positioned on a Z axis forming an axis of symmetry for the secondary ray collimator. A point 0 on the Z axis forms the origin of a Cartesian coordinate system. The primary ray collimator allows passage only of x-ray beams impinging on the point 0. The x-ray source has an extended anode with a focus position controlled electronically about the anode length. Primary ray collimator and x-ray source extend cylindrically symmetrically about the symmetry axis or parallel to the Y axis in the X-Y plane.
Abstract:
An apparatus for measuring the pulse transmission spectrum of elastically scattered quantities includes at least one diaphragm displaceable in a y-direction for switching between fine and coarse local resolution of the examined partial volumes of an examination object, wherein the diaphragm narrows the effective ray width transversely of a scanning direction, and a diaphragm system displaceable in a x-direction for limiting and extension of the partial volume in a z-direction, wherein the diaphragm system includes at least two circular ring diaphragms arranged one above the other and identical with respect to their circular ring structure, and wherein the circular ring diaphragms are arranged at a relative offset for reducing an effective imaging slot width or a detector slot width.
Abstract:
A patient table for radiation image exposure has a top surface forming a patient positioning surface that has an integrated solid-state radiation detector with a size substantially corresponding to the size of the patient positioning surface.