Abstract:
A method and apparatus (11) for irradiating an electron beam, wherein a triangular wave generator (22) provides a triangular wave current to a scanning coil (17) to move the electron beam in a first scanning direction (Y), while a square wave generator (21) provides a square wave current to a deflecting coil (16) to move the electron beam in a second scanning direction (X) orthogonal to the first scanning direction (Y). The triangular wave current provided from the triangular wave generator is modulated to cancel the effects of hysteresis in the scanning coil. Further, the rise of the square wave current is synchronized and shifted a prescribed interval in relation to the peak values of the triangular wave current in order to distribute the reversing points on the electron beam path along the second scanning direction.
Abstract:
By using a large area cathode, an electron source can be made that can irradiate a large area more uniformly and more efficiently than currently available devices. The electron emitter can be a carbon film cold cathode, a microtip or some other emitter. It can be patterned. The cathode can be assembled with electrodes for scanning the electron source.
Abstract:
A method and apparatus (11) for irradiating an electron beam, wherein a triangular wave generator (22) provides a triangular wave current to a scanning coil (17) to move the electron beam in a first scanning direction (Y), while a square wave generator (21) provides a square wave current to a deflecting coil (16) to move the electron beam in a second scanning direction (X) orthogonal to the first scanning direction (Y). The triangular wave current provided from the triangular wave generator is modulated to cancel the effects of hysteresis in the scanning coil. Further, the rise of the square wave current is synchronized and shifted a prescribed interval in relation to the peak values of the triangular wave current in order to distribute the reversing points on the electron beam path along the second scanning direction.
Abstract:
An industrial X-ray/electron beam source includes an accelerator having a) a coaxial cavity b) an electron gun for emitting an electron beam to be accelerated, c) at least one deflection magnet positioned outside of the cavity, and d) a radio frequency power supply means for supplying power of a radio frequency to the cavity to induce TM010 mode as an accelerating mode in the cavity; and a beam irradiator having a two-dimensional scanning magnet which deflects accelerated beam by the accelerator, an extracting window for extracting the deflected electron beam to be irradiated to an object, and means for guiding the deflected beam toward a center of the extracting window in a radial direction. The source is advantageous in that the electron beams do not intersect inside the cavity, which can reduce beam loss, and that beams or X-rays are irradiated to the object spatially uniformly.
Abstract:
A modular electron beam device is disclosed, the device being housed in a modular enclosure containing a power supply subsystem coupled to provide power to an electron beam tube. The enclosure is shaped to permit stacking of plural such modular units in a way that the stripe-shaped beam emitted from each of the units completely irradiates a surface to be treated. Beams may lie on different lines but the combined beams sweep out a width on a surface which is a continuous span. In an alternate embodiment of the invention, the modular unit comprises a plurality of electron beam units, each comprising an electron tube and a filament and bias supply to power the tube. A single high voltage stack is common to the plural tube/filament/bias sub-units. A daisy-chain arrangement allows for the single high voltage stack to power all of the tube units. In yet another embodiment, the modular unit comprises a plurality of electron tubes powered by a single power supply.
Abstract:
A vacuum tube electron beam device having a thin, single crystal, electron permeable, gas impermeable membrane for electron transmission and methods for making such a device. Single crystal membranes can have small thickness due to high strength, are highly transmissive to free electrons due to that small thickness. The ordered crystalline structure of such membranes provides minimal obstructions to electron beams, and yet is highly impermeable to penetration by gas and liquid molecules. Single crystals are anisotropically etched to precise membrane dimensions, and can also be etched to provide microchannel structures for flowing cooling fluid across the membrane during use. A doped silicon anode can provide support for the membrane with matching thermal expansion characteristics, and a crystalline anode can be integral with the membrane. A double membrane embodiment confines the cooling fluid so that it passes close to both membranes. A double membrane structure can also have a pressure between the membranes that is between the pressure within the vacuum tube and ambient pressure outside the vacuum tube, allowing the membranes to be thinner. The membrane can also be compressed for increased strength. A number of cooling methods are used to maintain the integrity of the membrane.
Abstract:
An electron beam source or generator is described for the treatment of toxic materials in a treatment system in which electron beams are reacted with a flowing influent in a reaction chamber. The system is modular allowing different configurations as demanded by the site and by the clean-up job. It is also portable in that it can be easily moved from place to place. If mounted on a movable base it can be taken from place to place for use.
Abstract:
A plasma X-ray tube, which can be referred to as a one-chamber ionizing tube for pre-ionizing TE lasers, in particular excimer lasers, includes an extended, box-like housing with a U-shaped hollow cathode which is disposed in the interior of the housing and is also elongated. The open side of the hollow electrode faces an X-ray target which is in the form of a gas-tight foil. Between the X-ray target and the hollow cathode is a long wire-shaped igniting electrode. When a positive voltage or a voltage pulse is applied to the igniting electrode, an electrical field is formed around it. Electrons that are present are forced onto a long, spiral path and gas atoms are ionized under the influence of the electrical field and because of ambient radiation. Electron avalanches form and lead to initiation of a wire discharge. When the accelerator voltage, which is typically at most between 60 kV and 120 kV, is applied to the hollow cathode low-pressure plasma, ions are extracted and accelerated against the hollow cathode. When the ions impact, secondary electrons are emitted from the hollow cathode and are accelerated in the opposite direction, so that an electron beam forms and strikes the X-ray target to generate X-ray retarding radiation. The plasma X-ray tube is fundamentally suitable as an electron gun, with a suitable electron-beam permeable configuration of a foil that covers the window opening in the target retaining wall and serves as an electron window.
Abstract:
A novel electron beam apparatus and technique wherein a plurality of longitudinally extending heated filaments is employed, each similarly offset laterally of a central longitudinal axis, but with successive filaments alternately disposed on opposite sides of said axis and cooperating with a first low velocity accelerating stage comprising staggered grid slots and openings, and a high velocity second accelerating stage to provide long uniform longitudinal electron beams.
Abstract:
A cold cathode electron gun utilizes a metallic torus for electrostatic focusing of an electron beam. A nonconductive tube is disposed within and along the axis of the torus. A conductive aerodynamic body electrically connected to the torus forms an annular venturi in the tube and includes a face which serves as a high field emitting surface. High molecular weight gas is introduced into a proximal end of the tube at a stagnation pressure sufficient to produce supersonic flow thereby causing a vacuous gas region adjacent the emitting surface. The torus and emitting surface are driven to a very high negative potential by a Tesla transformer or the like, producing high field emission into the vacuous region. The electric field of the torus produces, from the emitted electrons, an electron beam which issues from the tube into the atmosphere.