Varian Semiconductor Equipment Associates, Inc.

Applied Materials, Inc.

Jay Thomas Scheuer

Alexandre Likhanskii

Alexander S Perel

Bon-Woong Koo

Frank Sinclair

William Davis Lee

Peter F Kurunczi

Graham Wright

Costel Biloiu

Eric D Hermanson

Tseh-Jen Hsieh

Kevin R Anglin

Svetlana Radovanov

William M Holber

Daniel R Tieger

Robert C Lindberg

Ronald Johnson

You Chia Li

Jay S Johnson

Ryan Downey

Joseph C Olson

Neil J Bassom

Daniel Distaso

Bjorn O Pedersen

Ludovic Godet

Morgan Evans

Anthony Renau

Peter Lawrence Kellerman

Timothy J Miller

Craig Richard Chaney

Russell J Low

Christopher R Hatem

Steven Raymond Walther

Jonathan Gerald England

George Gammel

Antonella Cucchetti

Shardul Patel

Ziwei Fang

Eric D Wilson

Rajesh Dorai

Joseph P Dzengeleski

David P Sporleder

Harold M Persing

Brant S Binns

Bon Woong Koo

Nevin H Clay

Edmund Jacques Winder

Thomas Stacy

Chris Leavitt

Sudhakar Mahalingam

Tyler Wills

Sung-Cheon Ko

Ashwin Shetty

Kenneth Swenson

Erik A Mitchell

Xiangdong He

Provided herein are approaches for optimizing a full horizontal scanned beam distance of an accelerator beam. In one approach, a method may include positioning a first Faraday cup along a first side of an intended beam-scan area, positioning a second Faraday cup along a second side of the intended beam-scan area, scanning an ion beam along the first and second sides of the intended beam-scan area, measuring a first beam current of the ion beam at the first Faraday cup and measuring a second beam current of the ion beam at the second Faraday cup, and determining an optimal scan distance of the ion beam across the intended beam-scan area based on the first beam current and the second beam current.

Systems and methods for optimizing full horizontal scanned beam distance

An ion source capable of extracting a ribbon ion beam with improved uniformity is disclosed. One of the walls of the ion source has a protrusion on its interior surface facing the chamber. The protrusion creates a loss area that serves as a sink for free electrons and ions. This causes a reduction in plasma density near the protrusion, and may improve the uniformity of the ribbon ion beam that is extracted from the ion source by modifying the beam current near the protrusion. The shape of the protrusion may be modified to achieve the desired uniformity. The protrusion may also be utilized with a cylindrical ion source. In certain embodiments, the protrusion is created by a plurality of mechanically adjustable protrusion elements.

Device to control uniformity of extracted ion beam

Single-slot tubular cathode

An ion source having an extraction plate with a variable thickness is disclosed. The extraction plate has a protrusion on its interior or exterior surface proximate the extraction aperture. The protrusion increases the thickness of the extraction aperture in certain regions. This increases the loss area in those regions, which serves as a sink for ions and electrons. In this way, the plasma density is decreased more significantly in the regions where the extraction aperture has a greater thickness. The shape of the protrusion may be modified to achieve the desired plasma uniformity. Thus, it may be possible to create an extracted ion beam having a more uniform ion density. In some tests, the uniformity of the beam current along the width direction was improved by between 20% and 50%.

Variable thickness ion source extraction plate

An ion source capable of extracting a ribbon ion beam with improved vertical angular uniformity is disclosed. The extraction plate and extraction optics are designed such that there is at least one non-uniform gap between adjacent components. A non-uniform gap may be effective in reducing angular spread non-uniformity of the extracted ribbon ion beam. Specifically, for a given gap in the Z direction, ions extracted from regions with lower plasma density may have more vertical angular spread. A larger gap in the Z direction between components in this region may make the vertical angular spread closer to the vertical angular spread of ions extracted from regions with higher plasma density. The non-uniform gap may be created by having an extraction plate that is flat or curved and electrodes that are flat, convex or concave. In certain embodiments, the non-uniform gap is located between the extraction plate and the suppression electrode.

Mismatched optics for angular control of extracted ion beam

An ion source including a chamber housing defining an ion source chamber and including an extraction plate on a front side thereof, the extraction plate having an extraction aperture formed therein, and a tubular cathode disposed within the ion source chamber and having an opening formed in a front half thereof nearest the extraction aperture, wherein a rear half of the tubular cathode furthest from the extraction aperture is closed.

Ion source with single-slot tubular cathode

A beamline ion implanter and a method of operating a beamline ion implanter. A method may include performing an ion implantation procedure during a first time period on a first set of substrates, in a process chamber of the ion implanter, and performing a first pressure-control routine during a second time period by: introducing a predetermined gas to reach a predetermined pressure into at least a downstream portion of the beam-line for a second time period. The method may include, after completion of the first pressure-control routine, performing the ion implantation procedure on a second set of substrates during a third time period.

Particle yield via beam-line pressure control

Provided herein are approaches for in-situ plasma cleaning of ion beam optics. In one approach, a system includes a component (e.g., a beam-line component) of an ion implanter processing chamber. The system further includes a power supply for supplying a first voltage and first current to the component during a processing mode and a second voltage and second current to the component during a cleaning mode. The second voltage and current are applied to one or more conductive beam optics of the component, individually, to selectively generate plasma around one or more of the one or more conductive beam optics. The system may further include a flow controller for adjusting an injection rate of an etchant gas supplied to the beam-line component, and a vacuum pump for adjusting pressure of an environment of the beam-line component.

In-situ plasma cleaning of process chamber components

Provided herein are approaches for decreasing particle generation in an electrostatic lens. In some embodiments, an ion implantation system may include an electrostatic lens including an entrance for receiving an ion beam and an exit for delivering the ion beam towards a target, the electrostatic lens including a first terminal electrode, a first suppression electrode, and a first ground electrode disposed along a first side of an ion beamline, wherein the first ground electrode is grounded and positioned adjacent the exit. The electrostatic lens may further include a second terminal electrode, a second suppression electrode, and a second ground electrode disposed along a second side of the ion beamline, wherein the second ground electrode is grounded and positioned adjacent the exit. The implantation system may further include a power supply operable to supply a voltage and a current to the electrostatic lens for controlling the ion beam.

Electrostatic filter providing reduced particle generation

An ion source including a chamber housing defining an ion source chamber and including an extraction plate on a front side thereof, the extraction plate having an extraction aperture formed therein, and a tubular cathode disposed within the ion source chamber and having a slot formed in a front-facing semi-cylindrical portion thereof disposed in a confronting relationship with the extraction aperture, wherein a rear-facing semi-cylindrical portion of the tubular cathode directed away from the extraction aperture is closed.

An indirectly heated cathode ion source having a cylindrical housing with two open ends is disclosed. The cathode and repeller are sized to fit within the two open ends. These components may be inserted into the open ends, creating a small radial spacing that provides electrical isolation between the cylindrical housing and the cathode and repeller. In another embodiment, the repeller may be disposed from the end of the cylindrical housing creating a small axial spacing. In another embodiment, insulators are used to hold the cathode and repeller in place. This design results in a reduced distance between the cathode column and the extraction aperture, which may be beneficial to the generation of ion beams of certain species.

Cylindrical shaped arc chamber for indirectly heated cathode ion source

Provided herein are approaches for in-situ plasma cleaning of one or more components of an ion implantation system. In one approach, the component may include a beam-line component having one or more conductive beam optics. The system further includes a power supply for supplying a first voltage and first current to the component during a processing mode and a second voltage and second current to the component during a cleaning mode. The second voltage and current may be applied to the conductive beam optics of the component, in parallel, to selectively (e.g., individually) generate plasma around one or more of the one or more conductive beam optics. The system may further include a flow controller for adjusting an injection rate of an etchant gas supplied to the component, and a vacuum pump for adjusting pressure of an environment of the component.

Provided herein are approaches for in-situ plasma cleaning of one or more components of an ion implantation system. In one approach, the component may include a beam-line component, such as an energy purity module, having a plurality of conductive beam optics contained therein. The system further includes a power supply system for supplying a voltage and a current to the beam-line component during a cleaning mode, wherein the power supply system may include a first power plug coupled to a first subset of the plurality of conductive beam optics and a second power plug coupled to a second subset of the plurality of conductive beam optics. During a cleaning mode, the voltage and current may be simultaneously supplied and split between each of the first and second power plugs.

RF clean system for electrostatic elements

Methods for processing of a workpiece are disclosed. A fluid that contains a desired dopant is prepared. The workpiece is immersed in this fluid, such that the dopant is able to contact all surfaces of the workpiece. The fluid is then evacuated, leaving behind the dopant on the workpiece. The dopant is then subjected to a thermal treatment to drive the dopant into the surfaces of the workpiece. In certain embodiments, a selective doping process may be performed by applying a mask to certain surfaces prior to immersing the workpiece in the fluid. In certain embodiments, the fluid may be in a super-critical state to maximize the contact between the dopant and the workpiece.

Liquid immersion doping

Growing community of inventors

Rowley, MA, United States of America

Jay Thomas Scheuer