Abstract:
Methods and a system of an ion implantation system are disclosed that are capable of increasing beam current above a maximum kinetic energy of a first charge state from an ion source without changing the charge state at the ion source. Positive ions having a first positive charge state are selected into an accelerator. The positive ions of the first positive charge state are accelerated in acceleration stages and stripped to convert them to positive ions of a second charge state. A second kinetic energy level higher than the maximum kinetic energy level of the first charge state can be obtained.
Abstract:
An ion implantation system and associated method includes a scanner configured to scan a pencil shaped ion beam into a ribbon shaped ion beam, and a beam bending element configured to receive the ribbon shaped ion beam having a first direction, and bend the ribbon shaped ion beam to travel in a second direction. The system further includes an end station positioned downstream of the beam bending element, wherein the end station is configured to receive the ribbon shaped ion beam traveling in the second direction, and secure a workpiece for implantation thereof. In addition, the system includes a beam current measurement system located at an exit opening of the beam bending element that is configured to measure a beam current of the ribbon shaped ion beam at the exit opening of the beam bending element.
Abstract:
An implanter provides two-dimensional scanning of a substrate relative to an implant beam so that the beam draws a raster of scan lines on the substrate. The beam current is measured at turnaround points off the substrate and the current value is used to control the subsequent fast scan speed so as to compensate for the effect of any variation in beam current on dose uniformity in the slow scan direction. The scanning may produce a raster of non-intersecting uniformly spaced parallel scan lines and the spacing between the lines is selected to ensure appropriate dose uniformity.
Abstract:
An ion source assembly 10 is disclosed, the assembly comprising a source sub assembly having an ion source 20, an extraction electrode 40 and an electrically insulating high voltage bushing 60 to support the extraction electrode 40 relative to the ion source 20. The ion source assembly further includes a chamber 70 having an exit aperture to allow egress of ions to an ion implanter. The chamber 70 encloses one or more further electrodes 80,90. The source sub assembly is mounted to the chamber 70 via a hinge 150. This allows ready access to the inner walls of the chamber 70, which in turn allows easier maintenance and cleaning of the further electrodes 80,90 as well as the inner walls of the chamber 70. Preferably, a liner 160 is employed on the inner walls of the chamber 70.
Abstract:
A vaporizer system for an ion source includes a radiation source positioned on the vaporizer axis for providing radiation, multiple crucibles radially spaced from the axis and circumferentially spaced from each other and a reflector rotatable about the axis for directing radiation from the source at a selected one of the crucibles. The radiation causes heating of the selected crucible and vaporization of a solid source material contained therein. The radiation source is a visible and/or infrared emitting lamp such as a quartz halogen lamp. The crucibles are thermally isolated from each other by a heat shield so that the selected crucible is heated while the others remain relatively cool.
Abstract:
The present invention involves a beam energy identification system, comprising an accelerated ion beam, wherein the accelerated ion beam is scanned in a fast scan axis within a beam scanner, wherein the beam scanner is utilized to deflect the accelerated ion beam into narrow faraday cups downstream of the scanner, wherein a difference in scanner voltage or current to position the beam into the Faraday cups is utilized to calculated the energy of ion beam.
Abstract:
An ion beam uniformity control system, wherein the uniformity control system comprising a differential pumping chamber that encloses an array of individually controlled gas jets, wherein the gas pressure of the individually controlled gas jets are powered by a controller to change the fraction of charge exchanged ions, and wherein the charge exchange reactions between the gas and ions change the fraction of the ions with original charge state of a broad ion beam, wherein the charge exchanged portion of the broad ion beam is removed utilizing an deflector that generates a magnetic field, a Faraday cup profiler for measuring the broad ion beam profile; and adjusting the individually controlled gas jets based upon feedback provided to the controller to obtain the desired broad ion beam.
Abstract:
A ribbon ion beam system, comprising an ion source configured to generate a ribbon ion beam along a first beam path, wherein the ribbon ion beam enters a mass analysis magnet having a height dimension (h1) and a long dimension (w1) that is perpendicular to an xy plane, wherein the mass analysis magnet is configured with its momentum dispersive xy plane to receive the ribbon ion beam and to provide magnetic fields to transmit the ribbon ion beam along a second beam path, wherein the ribbon ion beam exiting the mass analysis magnet is divergent in the non-dispersive xz plane and convergent in the xy plane, a mass selection slit for receiving the divergent ribbon ion beam and selecting desired ion species of the ribbon ion beam exiting the mass analysis magnet, an angle correction device configured to receive the divergent ribbon ion beam exiting the mass selection slit into a parallel ribbon ion beam in the horizontal xz plane and a diverging ribbon ion beam in an xy plane along a third beam path, and wherein the parallel ribbon beam has a variable height (h2) and a long dimension, width (w2).
Abstract:
A ribbon ion beam system, comprising an ion source configured to generate a ribbon ion beam along a first beam path, wherein the ribbon ion beam enters a mass analysis magnet having a height dimension (h1) and a long dimension (w1) that is perpendicular to an xy plane, wherein the mass analysis magnet is configured with its momentum dispersive xy plane to receive the ribbon ion beam and to provide magnetic fields to transmit the ribbon ion beam along a second beam path, wherein the ribbon ion beam exiting the mass analysis magnet is divergent in the non-dispersive xz plane and convergent in the xy plane, a mass selection slit for receiving the divergent ribbon ion beam and selecting desired ion species of the ribbon ion beam exiting the mass analysis magnet, an angle correction device configured to receive the divergent ribbon ion beam exiting the mass selection slit into a parallel ribbon ion beam in the horizontal xz plane and a diverging ribbon ion beam in an xy plane along a third beam path, and wherein the parallel ribbon beam has a variable height (h2) and a long dimension, width (w2).
Abstract:
An implanter provides two-dimensional scanning of a substrate relative to an implant beam so that the beam draws a raster of scan lines on the substrate. The beam current is measured at turnaround points off the substrate and the current value is used to control the subsequent fast scan speed so as to compensate for the effect of any variation in beam current on dose uniformity in the slow scan direction. The scanning may produce a raster of non-intersecting uniformly spaced parallel scan lines and the spacing between the lines is selected to ensure appropriate dose uniformity.