Abstract: A media carrier, adapted to hold a plurality of pieces of magnetic media, is disclosed. This media carrier can be placed on the workpiece support, or platen, allowing the magnetic media to be processed. In some embodiments, the media carrier is designed such that only one side of the magnetic media is exposed, requiring a robot or other equipment to invert each piece of media in the carrier to process the second side. In other embodiments, the media carrier is designed such that both sides of the magnetic media are exposed. In this scenario, the media carrier is inverted on the platen to allow processing of the second side.

Abstract: A technique for limiting fault current transmission is disclosed. In one particular exemplary embodiment, the technique may be realized with a fault current limiter comprising a core having at least first easy axis and a hard axis; and a first coil wound around the core, the first coil configured to carry current. In some embodiment, the easy axis of the core may be aligned with H fields generated by the current transmitted through the first coil.

Abstract: A ribbon beam mass analyzer having a first and second solenoid coils and steel yoke arrangement. Each of the solenoid coils have a substantially “racetrack” configuration defining a space through which an ion ribbon beam travels. The solenoid coils are spaced apart along the direction of travel of the ribbon beam. Each of the solenoid coils generates a uniform magnetic field to accommodate mass resolution of wide ribbon beams to produce a desired image of ions generated from an ion source.

Abstract: In an ion implanter, an inert gas is directed at a cathode assembly near an ion source chamber via a supply tube. The inert gas is provided with a localized directional flow toward the cathode assembly to reduce unwanted concentrations of cleaning or dopant gases introduced into the ion source chamber, thereby reducing the effects of unwanted filament growth in the cathode assembly and extending the manufacturing life of the ion source.

Abstract: An energy contamination detection apparatus includes a membrane and a charge collection plate disposed at a distance from the membrane. The membrane is configured to receive an ion beam and allow a portion of the ion beam having energy levels above a desired energy level to pass therethrough toward the charge collection plate and absorb or reflect portions of the ion beam having energy levels at or below the desired energy level. A voltage source is electrically coupled to the charge collection plate for providing a bias voltage to the charge collection plate. A detection circuit is coupled to the charge collection plate and is configured to detect energy contamination based on an amount of charge collected on the charge collection plate.

Abstract: A melt of a material is cooled and a sheet of the material is formed in the melt. This sheet is transported, cut into at least one segment, and cooled in a cooling chamber. The material may be Si, Si and Ge, Ga, or GaN. The cooling is configured to prevent stress or strain to the segment. In one instance, the cooling chamber has gas cooling.

Abstract: A novel, technique: for manufacturing bit patterned media is disclosed. In one particular exemplary embodiment, the technique may be realized as a method for manufacturing hit pattern media. The technique, which may be realized as a method comprising: forming a non-catalysis region on a first portion of a catalysis layer; forming a non-magnetic separator on the non-catalysis region; and forming a magnetic active region on it second portion of the catalysis layer adjacent to the first portion of the catalysis layer.

Abstract: An implantation system includes an ion extraction plate having a set of apertures configured to extract ions from an ion source to form a plurality of beamlets. A magnetic analyzer is configured to provide a magnetic field to deflect ions in the beamlets in a first direction that is generally perpendicular to a principle axis of the beamlets. A mass analysis plate includes a set of apertures wherein first ion species having a first mass/charge ratio are transmitted through the mass analysis plate and second ion species having a second mass/charge ratio are blocked by the mass analysis plate. A workpiece holder is configured to move with respect to the mass analysis plate in a second direction perpendicular to the first direction, wherein a pattern of ions transmitted through the mass analysis plate forms a continuous ion beam current along the first direction at the substrate.

Abstract: A method of controlling deflection of a charged particle beam in an electrostatic lens includes establishing a symmetrical electrostatic lens configuration comprising a plurality of electrodes disposed at unadjusted positions that are symmetric with respect to the central ray trajectory with applied unadjusted voltages that create fields symmetric with respect to the central ray trajectory. A symmetric electric field is calculated corresponding to the set of unadjusted voltages. A plurality of lower electrodes is arranged at adjusted positions that are asymmetric with respect to the central ray trajectory. A set of adjusted voltages is obtained for the plurality of lower electrodes, wherein the set of adjusted voltages corresponds to a set of respective potentials of the symmetric electric field at respective adjusted asymmetric positions. The adjusted voltages are applied to the asymmetric lens configuration when the charged particle beam passes therethrough.

Abstract: An ion source is provided that utilizes the same dopant gas supplied to the chamber to generate the desired process plasma to also provide temperature control of the chamber walls during high throughput operations. The ion source includes a chamber having a wall that defines an interior surface. A liner is disposed within the chamber and has at least one orifice to supply the dopant gas to an inside of the chamber. A gap is defined between at least a portion of the interior surface of the chamber wall and the liner. A first conduit is configured to supply dopant gas to the gap where the dopant gas has a flow rate within the gap. A second conduit is configured to remove the dopant gas from the gap, wherein the flow rate of the dopant gas within the gap acts as a heat transfer media to regulate the temperature of the interior of the chamber.

Abstract: An ion source is provided that utilizes a cooling plate and a gap interface to control the temperature of an ion source chamber. The gap interface is defined between the cooling plate and a wall of the chamber. A coolant gas is supplied to the interface at a given pressure where the pressure determines thermal conductivity from the cooling plate to the chamber to control the temperature of the interior of the chamber.

Abstract: A system and method for maintain a desired degree of platen flatness is disclosed. A laser system is used to measure the flatness of a platen. The temperature of the platen is then varied to achieve the desired level of flatness. In some embodiments, this laser system is only used during a set up period and the resulting desired temperature is then used during normal operation. In other embodiments, a laser system is used to measure the flatness of the platen, even while the workpiece is being processed.

Abstract: A method of fabricating a workpiece is disclosed. A material defining apertures is applied to a workpiece. A species is introduced to the workpiece through the apertures and the material is removed. For example, the material may be evaporated, may form a volatile product with a gas, or may dissolve when exposed to a solvent. The species may be introduced using, for example, ion implantation or gaseous diffusion.

Abstract: A beam line ion implanter includes an ion source configured to generate an ion beam, a scanner configured to scan the ion beam to produce a scanned ion beam having trajectories which diverge from a scan origin, and a focusing element having a focusing field positioned upstream of the scanner configured to focus the ion beam to a focal point at the scan origin. A method of ion beam tuning includes generating an ion beam, focusing the ion beam to a focal point positioned at a scan origin, and scanning the ion beam to produce a scanned ion beam having trajectories which diverge from the scan origin.

Abstract: A technique for manufacturing hit pattern media is disclosed. In one particular exemplary embodiment, the technique may be realized as a method for manufacturing bit pattern media. The method may comprise forming an intermediate layer comprising a modified region and a first region adjacent to one another, where the modified region and the first region may have at least one different property; depositing magnetic species on the first region of the intermediate layer to form an active region; and depositing non-ferromagnetic species on the modified region of the intermediate layer to form a separator.

Abstract: An ion beam is generated and the energy of this ion beam is changed from a first energy to a second energy through, for example, acceleration or deceleration. A portion of the ion beam is blocked after the energy is changed and the ion beam is implanted into a workpiece. A plurality of blockers may be used to block the beam. Each blocker may be attached to a drive unit configured to translate one of the blockers in a first direction.

Abstract: A method and apparatus for controlling deflection, deceleration, and focus of an ion beam are disclosed. The apparatus may include a graded deflection/deceleration lens including a plurality of upper and lower electrodes disposed on opposite sides of an ion beam, as well as a control system for adjusting the voltages applied to the electrodes. The difference in potential between pairs of upper and lower electrodes are varied using a set of “virtual knobs” that are operable to independently control deflection and deceleration of the ion beam. The virtual knobs include control of beam focus and residual energy contamination, control of upstream electron suppression, control of beam deflection, and fine tuning of the final deflection angle of the beam while constraining the beam's position at the exit of the lens. In one embodiment, this is done by fine tuning beam deflection while constraining the beam position at the exit of the VEEF.

Abstract: A sheet of a material is disposed in a melt of the material. The sheet is formed using a cooling plate in one instance. An exciting coil and sensing coil are positioned downstream of the cooling plate. The exciting coil and sensing coil use eddy currents to determine a thickness of the solid sheet on top of the melt.

Abstract: Providing vapor to a vapor-receiving device housed in a high vacuum chamber. An ion beam implanter, as an example, has a removable high voltage ion source within a high vacuum chamber and a vapor delivery system that delivers vapor to the ion source and does not interfere with removal of the ion source for maintenance. For delivering vapor to a vapor-receiving device, such as the high voltage ion source under vacuum, a flow interface device is in the form of a thermally conductive valve block. A delivery extension of the interface device automatically connects and disconnects within the high vacuum chamber with the removable vapor receiving device by respective installation and removal motions. In an ion implanter, the flow interface device or valve block and source of reactive cleaning gas are mounted in a non-interfering way on the electrically insulating bushing that insulates the ion source from the vacuum housing and the ion source may be removed without disturbing the flow interface device.

Abstract: A sheet measurement apparatus has a sheet disposed in a melt. The measurement system uses a beam to determine a dimension of the sheet. This dimension may be, for example, height or width. The beam may be, for example, collimated light, a laser, x-rays, or gamma rays. The production of the sheet may be altered based on the measurements.