Hughes Aircraft Company

Varian Semiconductor Equipment Associates, Inc.

Varian Associates, Inc.

Charles M McKenna

William M Clark, Jr

Anthony Renau

Robert L Seliger

John L Bartelt

J William Ward

William L Johnson

Svetlana Radovanov

Paul J Murphy

Ka-Ngo Leung

Ross D Olney

Douglas A Brown

Edward W Bell

Bjorn O Pedersen

Nicholas R White

Jerg B Jergenson

Charles W Slayman

Malcom D Williams

Wulf B Kunkel

Peter E Maciejowski

James E Wood

Irwin R Sharapata

William G Goodenough

An ion implanter includes an ion source for generating an ion beam, an analyzer for separating unwanted components from the ion beam, a first beam transport device for transporting the ion beam through the analyzer at a first transport energy, a first deceleration stage positioned downstream of the analyzer for decelerating the ion beam from the first transport energy to a second transport energy, a beam filter positioned downstream of the first deceleration stage for separating neutral particles from the ion beam, a second beam transport device for transporting the ion beam through the beam filter at the second transport energy, a second deceleration stage positioned downstream of the beam filter for decelerating the ion beam from the second transport energy to a final energy, and a target site for supporting a target for ion implantation. The ion beam is delivered to the target site at the final energy. In a double deceleration mode, the second transport energy is greater than the final energy for highest current at low energy. In an enhanced drift mode, the second transport energy is equal to the final energy for highest beam purity at low energy.

Ion implanter having two-stage deceleration beamline

Methods and apparatus are provided for efficiently operating an ion implanter which includes a charged particle accelerator in a high energy mode and in a low energy mode. The charged particle accelerator includes a high voltage power supply, an accelerator column coupled to the high voltage power supply and a switching assembly. The accelerator column includes a plurality of accelerator electrodes. The high voltage power supply is disabled from energizing the accelerator column in the low energy mode. The switching assembly includes switching elements for electrically connecting the accelerator electrodes to a reference potential in the low energy mode and for electrically isolating the accelerator electrodes from the reference potential in the high energy mode. The switching assembly prevents positive potentials on the accelerator electrodes and thus minimizes space charge expansion of the beam when transporting positive ion beams in the low energy mode.

Methods and apparatus for operating high energy accelerator in low energy mode

An ion beam generator includes an ion beam source for generating an ion beam, an acceleration/deceleration column for selectably accelerating or decelerating ions in the ion beam to desired energies, a source filter positioned between the ion beam source and the acceleration/deceleration column for removing first undesired species from the ion beam, and a mass analyzer positioned downstream of the acceleration/deceleration column for removing second undesired species from the ion beam. The ion beam generator supplies an energetic ion beam having a low level of energy and mass contaminants. The ion beam generator may be utilized in an ion implanter.

Acceleration and analysis architecture for ion implanter

Methods and apparatus for neutralization of a workpiece such as a semiconductor wafer in a system wherein a beam of positive ions is applied to the workpiece. The apparatus includes an electron source for generating an electron beam and a magnetic assembly for generating a magnetic field for guiding the electron beam to the workpiece. The electron beam path preferably includes a first section between the electron source and the ion beam and a second section which is coincident with the ion beam. The magnetic assembly generates an axial component of magnetic field along the electron beam path. The magnetic assembly also generates a transverse component of the magnetic field in an elbow region between the first and second sections of the electron beam path. The electron source preferably includes a large area lanthanum hexaboride cathode and an extraction grid positioned in close proximity to the cathode. The apparatus provides a high current, low energy electron beam for neutralizing charge buildup on the workpiece.

Charge neutralization apparatus for ion implantation system

A masked ion beam lithography (MIBL) system and method is disclosed which is considerably more compact and economical than prior ion implantation devices. An H.sup.+ ion beam is extracted from a source in the form of an angularly expanding beam, and is transmitted through two lenses that sequentially accelerate the ions to energies in the range of 200-300 keV. The first lens focuses the beam so that it emerges from a crossover point with an amplified angular divergence at least three times the divergence of the initial beam, thereby considerably reducing the necessary column length. The second lens collimates the beam so that it can be directed onto a mask to expose resist on an underlying semiconductor substrate. A series of extraction electrodes are used to provide an initial point source beam with a desired angular expansion, and a specially designed sector magnet is positioned between the extraction mechanism and the first lens to remove particles heavier than H.sup.+ from the beam. Voltage ratios across the lenses and extraction electrodes can be varied in tandem, permitting control over the final beam energy by a simple voltage adjustment. The beam is aligned with the column axis and then steered into alignment with the mask channeling axis by a pair of octupole lenses.

Masked ion beam lithography system and method

U-shaped billet (52) has a slot (54) cut therein for receipt of a slip of insulator material (56). This body is machined on its front end (64) to produce a narrow bridge (66) of controlled cross-sectional area. Emitter needle (78) is positioned in a bore through the bridge to be heated by current through the bridge. The ion emitter body is rigid and strong to hold the emitter needle in the proper location.

Liquid metal ion source

An ion beam microfabrication system is described which is capable of operating in either a flooded beam mode, in which a relatively high current beam is used to yield a rapid throughput, or in a low current, high resolution focused ion beam mode. With a focused beam a small, relatively low current ion spot is deflected in a predetermined pattern over a portion of the wafer to produce more detailed patterning that is not achievable in the flooded beam mode. A lens is added to the beam column to modify the beam collimation between the focused and flooded modes, and switching between modes is accomplished by simply actuating or de-actuating the lens. The beam is formed with a larger acceptance angle and total current in the flooded than the focused mode.

Hybrid focused-flood ion beam system and method

A process for enhancing the wettability of evaporation elements, such as substrates and metal reservoirs used in liquid metal ion sources, and the elements so produced wherein a coating material is wettably coated onto the evaporation element at a coating temperature greater than the ion source operating temperature. The coated element is cooled to the operating temperature, and then contacted with the molten ion source alloy. The coating material is selected to wet the substrate or reservoir at the coating temperature, but to be itself wet by the ion source alloy at the ion source operating temperature. The preferred coating metal is gold, which is first applied by electrodeposition onto the evaporation element, and the evaporation element and coating are heated to a coating temperature of about 800.degree. C. to complete the coating step. The coated evaporation element is cooled to the source operating temperature of 200.degree. C.-300.degree. C. and dipped into the ion source alloy, which may be an alloy such as lead-gold-arsenic or lead-gold-antimony.

Enhanced wetting of liquid metal alloy ion sources

A liquid metal ion source alloy for high vapor pressure metalloids, wherein the alloy composition is chosen to have a low melting point so that the vapor pressure of the volatile constituents is low, even in the liquid state. Specifically, the ion source alloy is an alloy selected from the group of (Pb.sub.0.7-1.0 Au.sub.0.3-0).sub.0.7-0.99 (As+Sb).sub.0.3-0.01 and Pb.sub.0.20-0.30 Au.sub.0.45-0.55 (As+Sb).sub.0.20-0.30. The melting points of these alloys are about 200.degree. C.-300.degree. C., and the alloys may be maintained molten in contact with the emission elements for long periods of time without significant loss of the volatile species or reactivity with typical substrate materials used for emission elements.

Two lens focused ion beam column (10) has an accelerating lens (20) which carries a potential to focus an image of the liquid metal ion source (14) on the mass analyzer slit (26) with a magnification of about unity. Munro lens (36) accelerates the beam of selected ion species and demagnifies the image through a long working distance to provide an ion writing spot of less than about 1000 .ANG. size.

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Boxford, MA, United States of America

Charles M McKenna