Abstract:
Provided is an X-ray photographing apparatus including an X-ray source for generating and irradiating an X-ray; a collimator for controlling an X-ray photographing area to which an X-ray is irradiated by the X-ray source; a projector for generating and projecting a visible ray image by using image signals; a reflection mirror for reflecting the visible ray image projected by the projector to an X-ray photographing area; and a main controller for controlling the projector to match a light irradiation field corresponding to the visible ray image projected to the X-ray photographing area to the X-ray irradiation field.
Abstract:
An apparatus for forming a beam of energetic particles and for scanning the beam of particles with respect to an inspected object. The apparatus has a source of energetic particles characterized by an effective beam origin and a rotating hoop having at least one aperture, such that the effective beam origin of the source is closer to the inspected object than the axis of rotation of the rotating hoop. A collimating structure disposed interior to the rotating hoop collimates emission by the source into a fan beam prior to impinging on the rotating hoop. In some embodiments, the effective beam origin may be moved with respect to the axis of rotation of the hoop.
Abstract:
A positioning technique for aligning an X-ray lens (28) is described. A positioning apparatus (16) comprises a lens mounting component (44) and a positioning component (42). The positioning component (42) includes at least one goniometer stage (64, 66) having a centre of rotation that substantially coincides with the X-ray emitting portion (36) ("hot spot") of the X-ray source (12). The provision of one or more goniometer stages (64, 66) and, if required, one or more additional translation stages (60, 62) facilitates the adjustment of the X-ray lens (28) and makes the adjustment more intuitive.
Abstract:
An X-ray tube assembly (10) includes an anode (14), a cathode (12), and an X-ray transparent window (16). The anode (14) includes an X-ray-producing target (18) having a surface (20). The cathode (14) has an electron-beam axis (22) which intersects the target surface (20) at a focal point (24) and which is oriented at a first angle, (26) with respect to the target surface (20), of between and including fifteen and sixty degrees. The window (16) includes a surface (28) having a center point (30). A line between the focal and center points makes a second angle, with respect to the target surface (20), which is less than the first angle. A method for producing X-rays employs these angles.
Abstract:
An X-ray source comprises a thin film X-ray target (22) for generating X-rays in response to the application of electron beams, and a capillary tubular element (20) for allowing the X-rays to pass. The capillary tubular element (20) has such a diameter that the beams of the X-rays impinging on the inner surfaces of the capillary tubular element (20) are totally reflected. Additionally, a thin film (24) is provided for absorbing the electron beams, but allowing the X-rays to penetrate.
Abstract:
A scanning electron beam computed tomography scanner includes means defining a vacuum chamber (16), means (21, 22) for producing a space-charge limited electron beam (24) at one location in the chamber (16) and for directing it to a second location therein, and an elongate target (26) of the type which produces X-rays as a result of the impingement thereon by the electron beam (24). The scanner also includes an arrangement (42) at the second location for causing the beam (24) to scan along the length of the target (26) so as to impinge on the latter at all points along its length in order to cause X-rays to be produced by and emanate from the target (26). This arrangement includes means, specifically differential focal strength electron beam optics, for reducing the convergence of the electron beam (24) in the radial plane, at any instant, while maintaining the position of the waist of the beam (24) in the scan plane at the location of the target (26), thus reducing the mutual repulsion of the electrons in the beam and decreasing the azimuthal width of the electron beam spot. This also decreases the azimuthal width of X-ray beam effective focal spot and thereby improvesthe resolution of the scanner. The increased radial size of the electron beam spot is compensated by orienting the target (26) relative to the electron beam (24) in a specific way so that the axial width of the X-ray effective focal spot is independently controlled.
Abstract:
An electron beam production and control assembly especially suitable for use in producing X-rays in a computed tomography (CT) X-ray scanning system is disclosed herein along with its method of operation. This assembly produces its electron beam within a vacuum-sealed housing chamber which is evacuated of internal gases, except inevitably for small amounts of residual gas. The electron beam is produced by suitable means within the chamber and directed along a path therethrough from the chamber's rearwardmost end to its forwardmost end whereby to impinge on a suitable target for producing the necessary X-rays. Since there is residual gas within the chamber, the electrons of the beam will interact with it and thereby produce positive ions which have the effect of neutralizing the space charge of the electron beam. However, there are a number of differentiel arrangements disclosed herein which form part of the overall assembly for acting on these ions and reducing the neutralizing effectthey would otherwise have on the beam.
Abstract:
A method and apparatus for generating an electron beam using a new and improved plasma cathode system, the electron beam being suitable for use, by way of example, in large area pulsed x-ray devices of the type used for preionization of the discharge volume in certain lasers. The plasma cathode includes an electrically conductive member 12, 17 surrounded by an insulating sleeve 11 with an outer electrically conductive member 13, the first-mentioned member 12, 17 and a remote anode 16 being at ground potential, while the outer member 13 is maintained at a high negative potential relative to the first-mentioned member 12, 17 and the anode 16.