Abstract:
An electron beam production and control assembly especially suitable for use in producing X-rays in a computed tomography X-ray scanning system is disclosed herein. In this system, an electron beam is ultimately directed onto an X-ray producing target in a converging manner using electromagnetic components to accomplish this. The system also includes an arrangement for neutralizing the converging beam in a controlled manner sufficientto cause itto converge to a greater extent than it otherwise would in the absence of controlled neutralization, whereby to provide ion aided focusing.
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:
An electron beam production and control assembly especially suitable for use in producing X-rays in a computed tomography X-ray scanning system is disclosed herein. In this system, an electron beam is ultimately directed onto an X-ray producing target in a converging manner using electromagnetic components to accomplish this. The system also includes an arrangement for neutralizing the converging beam in a controlled manner sufficientto cause itto converge to a greater extent than it otherwise would in the absence of controlled neutralization, whereby to provide ion aided focusing.
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.