Veeco Instruments Inc.

Vebco Instruments Inc.

Rustam Yevtukhov

Alan V Hayes

Viktor Kanarov

Boris L Druz

Daniel Yakovlevitch

Peter Porshnev

Ira Reiss

Hari S Hegde

Kurt E Williams

Roger P Fremgen

Robert G Hieronymi

Rhodri Elliott

Adrian Celaru

Mathew Levoso

Carlos Fernando De Mello Borges

James M Best, Jr

Renga Rajan

The presently disclosed ion sources include one or more electromagnets for changing the distribution of plasma within a discharge space of an ion source. At least one of the electromagnets is oriented about an outer periphery of a tubular sidewall of the ion source and changes a distribution of the plasma in a peripheral region of the discharge space.

Ion sources and methods for generating ion beams with controllable ion current density distributions over large treatment areas

Embodiments relate to a grid short clearing system is provided for gridded ion beam sources used in industrial applications for materials processing systems that reduces grid damage during operation. In various embodiments, the ion source is coupled to a process chamber and a grid short clearing system includes methods for supplying a gas to the process chamber and setting the gas pressure to a predetermined gas pressure in the range between 50 to 750 Torr, applying an electrical potential difference between each adjacent pair of grids using a current-limited power supply, and detecting whether or not the grid shorts are cleared. The electrical potential difference between the grids is at least 10% lower than the DC electrical breakdown voltage between the grids with no contaminants.

Ion beam materials processing system with grid short clearing system for gridded ion beam source

Ion sources and methods for generating an ion bean with a controllable ion current density distribution. The ion source includes a discharge chamber having an optical grid position proximate at a first end and a re-entrant vessel positioned proximate a second end that opposes the first end. A plasma shaper extends from the re-entrant vessel and into the plasma discharge chamber. A position of the plasma shaper is adjustable relative to the grid-based ion optic such that the plasma shaper may operably change a plasma density distribution within the discharge chamber.

Ion sources and methods for generating an ion beam with controllable ion current density distribution

Methods of operating an electromagnet of an ion source for generating an ion beam with a controllable ion current density distribution. The methods may include generating plasma in a discharge space of the ion source, generating and shaping a magnetic field in the discharge space by applying a current to an electromagnet that is effective to define a plasma density distribution, extracting an ion beam from the plasma, measuring a distribution profile for the ion beam density, and comparing the actual distribution profile with a desired distribution profile for the ion beam density. Based upon the comparison, the current applied to the electromagnet may be adjusted either manually or automatically to modify the magnetic field in the discharge space and, thereby, alter the plasma density distribution.

Methods of operating an electromagnet of an ion source

Ion sources and methods for generating an ion beam with a controllable ion current density distribution. The ion source includes a discharge chamber and an electromagnet adapted to generate a magnetic field for changing a density distribution of the plasma inside the discharge chamber and, thereby, to change the ion current density distribution.

Ion sources and methods for generating an ion beam with a controllable ion current density distribution

A charged particle apparatus, with multiple electrically conducting semispheric grid electrodes, the grid electrodes mounted in a dielectric mounting ring, with hidden areas or regions to maintain electrical isolation between the grid electrodes as sputter deposits form on the grid electrodes and mounting ring. The grid electrodes are mounted to the mounting ring with slots and fastening pins that allow sliding thermal expansion and contraction between the grid electrodes and mounting ring while substantially maintaining alignment of grid openings and spacing between the grid electrodes. Asymmetric fastening pins facilitate the sliding thermal expansion while restraining the grid electrodes. Electrical contactors supply and maintain electrical potentials of the grid electrodes with spring loaded sliding contacts, without substantially affecting the thermal characteristics of the grid electrodes.

Charged particle beam extraction and formation apparatus

A charged particle source utilizes a novel plasma processing chamber, RF coil and ion optics, to achieve high uniformity. The plasma processing chamber has a re-entrant vessel which is movable, and which includes extensions of adjustable shape or position, to make more uniform the plasma contained within the chamber. One or more magnets, which may be static or moving, may be included within the re-entrant vessel. The ion optics include a grid with a number of apertures, and tuning features each surrounding an aperture. These tuning features either reduce the diameter of the associated aperture, or increase the length of that aperture, to create more uniform beamlets emerging from the grid. The RF coil includes a flux concentrator positioned adjacent to the winding in at least one angular region thereof to tune the magnetic field produced thereby.

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Briarwood, NY, United States of America

Rustam Yevtukhov