Abstract:
Multi-energy radiation sources comprising charged particle accelerators driven by power generators providing different RF powers to the accelerator, capable of interlaced operation, are disclosed. Automatic frequency control techniques are provided to match the frequency of RF power provided to the accelerator with the accelerator resonance frequency. In one example where the power generator is a mechanically tunable magnetron, an automatic frequency controller is provided to match the frequency of RF power pulses at one power to the accelerator resonance frequency when those RF power pulses are provided, and the magnetron is operated such that frequency shift in the magnetron at the other power at least partially matches the resonance frequency shift in the accelerator when those RF power pulses are provided. In other examples, when the power generator is a klystron or electrically tunable magnetron, separate automatic frequency controllers are provided for each RF power pulse. Methods and systems are disclosed.
Abstract:
In one example embodiment, an x-ray tube comprises an anode configured to rotate at an operating frequency, and a bearing assembly configured to rotatably support the anode and tuned to a resonant frequency that is different than the operating frequency.
Abstract:
A method of joining a first component and a second component is provided. The first component has a surface that comprises at least about 75% by volume of a refractory metal. The second component has a coefficient of thermal expansion greater than a coefficient of thermal expansion of the first component. The method includes disposing a coating on the surface of the first component. The coating includes an adhesion layer and a wetting layer disposed over the adhesion layer. The method further includes disposing a bonding material between the first and second components and joining them. The bonding material has a melting temperature lower than a melting temperature of the second component. An article made using the method is also presented.
Abstract:
In an x-ray system and a method for tomosynthetic scanning of a subject, x-ray radiation is emitted from two x-ray sources that are panned along a line relative to the subject during a tomosynthetic scan. The two x-ray sources are located next to each other along the line, and each emit an x-ray beam. X-rays from the two parallel beams attenuated by the subject are detected by a two-dimensional x-ray detector, that is substantially stationary during the tomosynthetic scan.
Abstract:
Systems and methods for detecting an image of an object by use of X-ray beams generated by multiple small area sources are disclosed. A plurality of monochromator crystals may be positioned to intercept the plurality of first X-ray beams such that a plurality of second X-ray beams each having predetermined energy levels is produced. Further, an object to be imaged may be positioned in paths of the second x-ray beams for transmission of the second X-ray beams through the object and emitting from the object a plurality of transmission X-ray beams. The X-ray beams may be directed at angles of incidence upon a plurality of analyzer crystals for detecting an image of the object.
Abstract:
An x-ray target pedestal assembly and a method of protecting the x-ray target from breaking down as a result of the extreme heat that is produced when an electron beam is aimed at the target to produce x-rays. The target is submerged in cooling fluid and is rotated by a constant flow of the cooling fluid over and around the target in order to dissipate heat. The fluid is guided by integrated flow diverters in the target cover. The target may also be protectively coated either in its entirety or along the electron beam path in order to further protect it from the heat of the electron beam impact or from breakdown as a result of attack of free radicals or other chemically reactive components of the cooling fluid which are produced in the extreme target environment.
Abstract:
A method for obtaining a concentrated, monochromatic x-ray beam from a standard x-ray tube or other source of polychromatic emission. X-rays from the anode of the x-ray tube fluoresce an adjoining, independent target that produces a monochromatic spectrum, a portion of which is focused by the x-ray optical system. This two-stage method gives the system considerably versatility without undue loss in signal. The two-stage concentrator makes practical the use of focusing optics in hand-held and portable instruments.
Abstract:
There is disclosed a device including: an electron beam generation device 10 which accelerates a pulse electron beam 1 to transmit the beam through a predetermined rectilinear orbit 2; a laser generation device 20 which generates a pulse laser light 3; a laser light introduction device 30 which introduces the pulse laser light 3 onto the rectilinear orbit 2 so as to collide with the pulse electron beam 1; a metal target 42 which generates a particular X-ray 5 by collision with the pulse electron beam 1: and a target moving device 40 capable of moving the metal target between a collision position 2a on the rectilinear orbit and a retreat position out of the orbit. A collision surface of the metal target 42 is positioned spatially at the same position as that of the collision point 2a. At the retreat position of the metal target, the pulse electron beam 1 collides with the pulse laser light 3 to generate a monochromatic hard X-ray 4. At the collision position of the metal target 42, the pulse electron beam 1 collides with the metal target 42 to generate the particular X-ray 5 from the same light source position 2a.
Abstract:
An anode for an X-ray source is formed in two parts, a main part and a collimating part. The main part has the target region formed on it. The two parts between them define an electron aperture through which electrons pass to reach the target region, and an X-ray aperture through which the X-rays produced at the target leave the anode. The anode produces at least the first stage of collimation of the X-ray beam produced.
Abstract:
According to one aspect of the present invention, a substrate processing system is provided. The system may include a chamber wall enclosing a chamber, a substrate support positioned within the chamber to support a substrate, an electromagnetic radiation source to emit electromagnetic radiation onto the substrate on the substrate support, the electromagnetic radiation causing photoelectrons to be emitted from a material on the substrate, an analyzer to capture the photoelectrons emitted from the substrate, and a magnetic field generator to generate a magnetic field within the chamber and guide the photoelectrons from the substrate to the analyzer.