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 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:
Several examples of a method for processing a substrate are disclosed. In a particular embodiment, the method may include: disposing a substrate having an upper surface and a lower surface on a platen contained in a chamber; generating a plasma containing a plurality of charged particles above the upper surface of the substrate, the plasma having a cross sectional area equal to or greater than a surface area of the upper surface of the substrate; applying a first bias voltage to the substrate to attract the charged particles toward the upper surface of the substrate; introducing the charged particles to a region extending under entire upper surface of the substrate; and initiating, concurrently, a first phase transformation in the region from the amorphous phase to a crystalline phase.
Abstract:
Techniques for measuring and controlling ion beam angle and density uniformity are disclosed. In one particular exemplary embodiment, the techniques may be realized as an apparatus for measuring and controlling ion beam angle and density uniformity. The apparatus may include a measuring assembly having an opening, a cup, and at least one collector at the rear of the cup. The apparatus may further include an actuator to move the measuring assembly along an actuation path to scan an ion beam to measure and control ion beam uniformity.
Abstract:
Techniques for commensurate cusp-field for effective ion beam neutralization are disclosed. In one particular exemplary embodiment, the techniques may be realized as a charged particle injection system comprising a beamguide configured to transport an ion beam through a dipole field. The charged particle injection system may also comprise a first array of magnets and a second array of magnets configured to generate a multi-cusp magnetic field, positioned along at least a portion of an ion beam path, the first array of magnets being on a first side of the ion beam path and the second array of magnets being on a second side of the ion beam path. The charged particle injection system may further comprise a charged particle source having one or more apertures configured to inject charged particles into the ion beam path. The charged particle injection system may furthermore align the one or more apertures with at least one of the first array of magnets and the second array of magnets to align the injected charged particles from the charged particle source with one or more magnetic regions for an effective charged particle diffusion into the ion beam path.
Abstract:
Techniques for providing optical ion beam metrology are disclosed. In one particular exemplary embodiment, the techniques may be realized as an apparatus for controlling beam density profile, the apparatus may include one or more camera systems to capture at least one image of an ion beam and a control system coupled to the one or more camera systems to control a beam density profile of the ion beam. The control system may further include a dose profiler to provide information to one or more ion implantation components in at least one of a feedback loop and a feedforward loop to improve dose and angle uniformity.
Abstract:
Electrical charge neutralization effects are known to be factors that affect the dose or concentrations of beam treatment by high current implanters. Raising beam energies to 1 MeV and beyond requires an understanding of the effects of both charge stripping and charge neutralization as well as a numerically efficient model compensating for these effects. Charge stripping generates ions of a higher charge state and may cause the measured electronic current from a Faraday cup to overestimate the true particle current. An analysis is based on the concept of an effective charge state for an ion beam and results in a more general interpretation that covers both the charge stripping effect as well as ion neutralization. Dose control using the techniques requires two adjustable parameters: an apparent cross section of interaction between the beam and particles in the beam path and the ratio of the final steady charge state to the initial charge state.
Abstract:
An ion implantation device is equipped with a high-speed driving device which causes rotation of a disk that supports semiconductor wafers around its outer periphery. A center position of the disk is the axis of the high-speed rotation. A low-speed driving device causes relative movement of the disk in a radial direction. The ion implantation device calculates the movement speed of the low-speed driving device with reference to different spacings between wafers about the outer periphery and the distance from the center of the disk to the ion implantation position and controls the low speed scan speed so that ions are uniformly implanted into the wafers.
Abstract:
This sheet production apparatus comprises a vessel defining a channel configured to hold a melt. The melt is configured to flow from a first point to a second point of the channel. A cooling plate is disposed proximate the melt and is configured to form a sheet on the melt. A spillway is disposed at the second point of the channel. This spillway is configured to separate the sheet from the melt.
Abstract:
A plasma processing apparatus and method are disclosed which create a uniform plasma within an enclosure. In one embodiment, a conductive or ferrite material is used to influence a section of the antenna, where a section is made up of portions of multiple coiled segments. In another embodiment, a ferrite material is used to influence a portion of the antenna. In another embodiment, plasma uniformity is improved by modifying the internal shape and volume of the enclosure.