Abstract:
A method of measuring a momentum transfer spectrum of elastically scattered X-ray quanta which emanate from a scatter voxel inside an object to be examined is described. A scatter voxel emits X-radiation in an X-direction and has a primary collimator which allows through only primary radiation aimed at a single isocentre at the origin of a Cartesian coordinates system. The X-ray quanta are emitted at an angle of scatter (Θ) with a constant Z-component (Θz). The method includes simultaneous recording of the energy spectrum of scatter quanta from the scatter voxel at different angles of scatter (Θ) with a spatially-resolving and energy-resolving detector in the Y-Z plane, determining the momentum transfer from the geometric data of the radioscopy unit for different angles of scatter (Θ), and combining respective diffraction profiles belonging to different angles of scatter (Θ) to produce a total-diffraction profile.
Abstract translation:描述了测量从被检查物体内的散射体素产生的弹性散射X射线量子的动量传递光谱的方法。 散射体素沿X方向发射X射线,并且具有主准直器,其允许仅通过瞄准在笛卡尔坐标系原点处的单个等中心的主辐射。 X射线量子以散射角(Theta)以恒定的Z分量(Theta z z)发射。 该方法包括使用散射体素以不同的散射角(Theta)与YZ平面中的空间分辨和能量分辨检测器同时记录散射量子的能量谱,从辐射检查的几何数据确定动量传递 用于不同散射角(Theta)的单位,并且组合属于不同散射角(Theta)的各个衍射曲线以产生总衍射分布。
Abstract:
A device for generating X-rays having a source for emitting electrons accommodated in a vacuum space, a liquid metal for emitting X-rays as a result of the incidence of electrons, and a pump for causing a flow of the liquid metal through a constriction where the electrons emitted by the source impinge upon the liquid metal, the constriction having a cross-sectional area which, seen in a flow direction, increases so that during operation in the flow direction, a decrease of a flow velocity takes place such that a decrease of a pressure of the liquid metal in the constriction, caused by viscous flow losses, substantially corresponds with an increase of the pressure caused by the decrease of the velocity so that a uniform and relatively low mechanical load is exerted on a window separating the constriction from the vacuum space during operation.
Abstract:
The invention relates to a device (1) for generating X-rays (57). The device comprises a source (7) for emitting electrons (53) and a liquid metal for emitting X-rays as a result of the incidence of electrons. The device further comprises a displacing member (11) for displacing the liquid metal through an impingement position (55) where the electrons emitted by the source impinge upon the liquid metal. As a result of the flow of liquid metal through the impingement position the heat, which is generated in the impingement position as a result of the incidence of the electrons upon the liquid metal, is transported away from the impingement position.According to the invention, the displacing member (11) has a contact surface (61), which is in contact with the liquid metal in the impingement position (55), and a driving member (31) for moving the contact surface in a direction which, in the impingement position, is substantially parallel to the contact surface. Thus the flow of liquid metal in the impingement position is achieved as a result of viscous shear forces in the liquid metal caused by friction forces between the liquid metal and the moving contact surface. As a result, the necessary pressure of the liquid metal is limited.
Abstract:
The invention relates to an X-ray source for generating substantially monochromatic fluorescent X-rays by means of a primary and a secondary target. The radiation source is characterized in that the primary target (10) is a liquid metal or a liquid metal alloy which is conducted between a first window (2) which is transparent to an electron beam and a second window (6) which is transparent to X-rays and is adjoined by the secondary target (11) in such a manner that the electrons which are incident on the primary target via the first window produce X-rays which have a maximum energy which corresponds essentially to an absorption edge of the secondary target when they reach the secondary target, so that substantially monochromatic fluorescent X-rays are excited in the secondary target.
Abstract:
A computed tomography apparatus includes a scanning unit which is rotatable relative to an examination zone, about an axis of rotation extending through the examination zone, a radiation source for generating a radiation beam, a diaphragm arrangement which is arranged between the radiation source and the examination zone in order to form a fan beam traversing the examination zone from the radiation beam, and a two-dimensional detector arrangement including a plurality of detector elements and a part of the measuring surface of which detects primary radiation from the fan beam whereas another part of its measuring surface detects scattered radiation produced in the examination zone. Perfect acquisition of the momentum transfer spectrum is achieved in that a collimator arrangement with a plurality of lamellas is arranged between the examination zone and the detector arrangement. The lamellas preferably are situated in planes that intersect each other at the focus of the radiation source and subdivide the fan beam into a number of segments so that the detector elements present in a column extending parallel to the axis of rotation are struck by primary radiation or scattered radiation from the same segment.
Abstract:
A method of detecting an object in an examination zone is well-suited for detecting land mines buried in the soil. The mean atomic numbers of the object is different from that of the examination zone. The examination zone is irradiated by gamma radiation. The annihilation radiation thus generated is measured and evaluated. The gamma radiation, which is sufficiently strong to generate electron-positron pairs, amounts to less than 10 MeV. The radiation generated in the examination zone by the gamma radiation beam is detected by a plurality of detector elements, which are arranged in such a manner that they can always detect only a respective segment of the gamma radiation beam.
Abstract:
The invention relates to a method of generating slice images of an examination zone which is irradiated by X-rays from a plurality of radiation source positions in order to generate separate single images, each associated with a difficult one of the source position for each single image there being stored image values which correspond to the absorption in its image points, slice images being generated in that slice image values are derived from the image values of the image points of the single images which are geometrically associated with a slice image point. This may give rise to contrast reversal and pseudo-resolution effects. These effects are eliminated in that the slice image values are derived by a weighted summing operation where the weighting factor applied to the image values of the single images enter the summing operation decreases as the distance between the radiation source position associated with the single image a central radiation source position increases.
Abstract:
A device for measuring the pulse transfer spectrum of X-ray quanta, includes a polychromatic X-ray source and an energy-resolving detector device for the scattered X-ray quanta. A secondary diaphragm device, arranged between the examination zone in which the object whose pulse transfer spectrum is to be determined is situated, and the detector device ensure on the one that each detector element of the detector device can detect scattered radiation only at a comparatively accurately defined scatter angle, and that the scatter angles of the various detector elements do not excessively deviate from one another.
Abstract:
Devices that measure the electron density in a body by means of radiation scattered from a narrow pencil beam of penetrating radiation directed through the body, produce defective images on reconstruction of the density distribution because of multiple scattering of radiation. This can of course be reduced by scattered ray diaphragms, but cannot be eliminated entirely. The invention therefore provides a means for detecting the size of the multiple scattered radiation component be measurement. For this purpose, the detector array which measures radiation including the single scattered radiation, is screened, at least osscasionally, from the single scattered radiation and the detected intensity values measured by the detector elements when so screened, are used to correct the values generated by measuring the detected radiation including the single scattered radiation.
Abstract:
A method for correcting an X-ray diffraction (XRD) profile measured by an X-ray diffraction imaging (XDi) system is provided. The XDi system includes an anode, a detector, and a control system. The method includes obtaining an emission spectrum of the anode using the control system. The emission spectrum includes spectral structures. The method further includes calculating a piecewise spectral-correction function using the spectral structures in the emission spectrum, obtaining a measured spectrum of an object, and applying the spectral-correction function to the measured spectrum to generate a spectrally-corrected measured spectrum.