Abstract: Disclosed is an inductively coupled RF plasma source that provides both magnetic confinement to reduce plasma losses and Faraday shielding to suppress parasitic capacitive components. The inductively coupled RF plasma system comprises an RF power source, plasma chamber, an array of permanent magnets, and an antenna array. The plasma chamber is comprised of walls and a dielectric window having an inner and outer surface wherein the inner surface seals the volume of the plasma chamber. The array of parallel conductive permanent magnets is electrically interconnected and embedded within the dielectric window walls proximate to the inner surface and coupled to ground on one end. The permanent magnet array elements are alternately magnetized toward and away from plasma in the plasma chamber to form a multi-cusp magnetic field. The antenna array may be comprised of parallel tubes through which an RF current is circulated. The antenna array is oriented perpendicular to the permanent magnet array.

Abstract: An ion source includes an ion source chamber, a cathode disposed within the ion source chamber and configured to emit electrons to generate an arc plasma, and a repeller configured to repell electrons back into the arc plasma. The ion source chamber and cathode may comprise a refractory metal. The ion source chamber further includes a gas source configured to provide a halogen species to the ion source chamber. The reactive insert is interoperative with the halogen species to yield a first etch rate of the refractory metal material within the ion source chamber under a first set of operating conditions that is less than a second etch rate of the refractory metal material within the ion source chamber under the first set of operating conditions when the reactive insert is not disposed within the ion source chamber.

Abstract: A processing apparatus may include a plasma source coupled to a plasma chamber to generate a plasma in the plasma chamber, an extraction plate having an aperture disposed along a side of the plasma chamber; a deflection electrode disposed proximate the aperture and configured to define a pair of plasma menisci when the plasma is present in the plasma chamber; and a deflection electrode power supply to apply a bias voltage to the deflection electrode with respect to the plasma, wherein a first bias voltage applied to the deflection electrode is configured to generate a first angle of incidence for ions extracted through the aperture from the plasma, and a second bias voltage applied to the deflection electrode is configured to generate a second angle of incidence of ions extracted through the aperture from the plasma, the second angle of incidence being different from the first angle of incidence.

Abstract: A hardware interlock system for monitoring operation of RF plasma sources. The hardware interlock system includes an RF generator operative to transmit a forward RF power used to generate plasma in a plasma chamber. A derivative based hardware interlock circuit is coupled in series with the RF generator. The derivative based hardware interlock circuit determines a reflected RF power derivative value indicative of the speed of change in reflected RF power values in the RF plasma ion source. An analog/digital (A/D) logic circuit is coupled with the derivative based hardware interlock circuit. The A/D logic circuit can shut down the RF generator output when the reflected RF power derivative value exceeds a threshold.

Abstract: In one embodiment an apparatus to provide electrons to a substrate includes a plurality of helicon plasma sources arranged in a helicon source array, wherein each helicon plasma source comprises a helical antenna configured to generate a wave vector parallel to a first axis; and a magnet configured to generate a magnetic field vector parallel to the first axis, wherein each helicon plasma source is further configured to generate a respective magnetic field vector that is opposite that of a magnetic field vector of an adjacent helicon plasma source.

Abstract: A plasma processing apparatus and method are disclosed which allows switching between the E and H operation modes and also increase the coupling efficiency of the RF power to the plasma. This apparatus may increase plasma density by a factor of about 1.25-1.65 for a given power output. Simultaneously, due to the high efficiency, the need to cool the antenna may be eliminated. A new antenna geometry which increases the amount of surface area for a given volume is used to take advantage of skin effects associated with RF electric current. In some embodiments, the antenna has a single turn to reduce proximity effects. The antenna may also be embedded in a ferrite material to further optimize its performance.

Abstract: An ion source includes an ion source chamber, a cathode disposed within the ion source chamber and configured to emit electrons to generate an arc plasma, and a repeller configured to repell electrons back into the arc plasma. The ion source chamber and cathode may comprise a refractory metal. The ion source chamber further includes a gas source configured to provide a halogen species to the ion source chamber. The reactive insert is interoperative with the halogen species to yield a first etch rate of the refractory metal material within the ion source chamber under a first set of operating conditions that is less than a second etch rate of the refractory metal material within the ion source chamber under the first set of operating conditions when the reactive insert is not disposed within the ion source chamber.

Abstract: A wide ion beam source includes a plurality of RF windows arranged in a predetermined relationship, a single plasma chamber disposed on a first side of the plurality of RF windows, a plurality of RF antennas, each RF antenna of the plurality of RF antennas disposed on a second side of a respective RF window of the plurality of RF windows, the second side being opposite the first side, and a plurality of RF sources, each RF source coupled to a respective RF antenna of the plurality of RF antennas, wherein a difference in frequency of a first RF signal produced by a first RF source coupled to a first RF antenna from that of a second RF signal produced by a second RF source coupled to an RF antenna adjacent to the first RF antenna is greater than 10 kHz.

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.

Abstract: A wide ion beam source includes a plurality of RF windows arranged in a predetermined relationship, a single plasma chamber disposed on a first side of the plurality of RF windows, a plurality of RF antennas, each RF antenna of the plurality of RF antennas disposed on a second side of a respective RF window of the plurality of RF windows, the second side being opposite the first side, and a plurality of RF sources, each RF source coupled to a respective RF antenna of the plurality of RF antennas, wherein a difference in frequency of a first RF signal produced by a first RF source coupled to a first RF antenna from that of a second RF signal produced by a second RF source coupled to an RF antenna adjacent to the first RF antenna is greater than 10 kHz.

Abstract: In one embodiment, a method for generating an ion beam having gallium ions includes providing at least a portion of a gallium compound target in a plasma chamber, the gallium compound target comprising gallium and at least one additional element. The method also includes initiating a plasma in the plasma chamber using at least one gaseous species and providing a source of gaseous etchant species to react with the gallium compound target to form a volatile gallium species.

Abstract: An ion source, capable of generating high-density wide ribbon ion beam, utilizing inductively coupled plasma production is disclosed. As opposed to conventional ICP sources, the present disclosure describes an ICP source which is not cylindrical. Rather, the source is defined such that its width, which is the dimension along which the beam is extracted, is greater than its height. The depth of the source may be defined to maximize energy transfer from the antenna to the plasma. In a further embodiment, a multicusp magnetic field surrounding the ICP source is used to further increase the current density and improve the uniformity of the extracted ion beam. Ion beam uniformity can also be controlled by means of several independent controls, including gas flow rate, and input RF power.

Abstract: A plasma processing apparatus and method are disclosed which allows switching between the E and H operation modes and also increase the coupling efficiency of the RF power to the plasma. This apparatus may increase plasma density by a factor of about 1.25-1.65 for a given power output. Simultaneously, due to the high efficiency, the need to cool the antenna may be eliminated. A new antenna geometry which increases the amount of surface area for a given volume is used to take advantage of skin effects associated with RF electric current. In some embodiments, the antenna has a single turn to reduce proximity effects. The antenna may also be embedded in a ferrite material to further optimize its performance.

Abstract: An RF ion source utilizing a heating/RF-shielding element for controlling the temperature of an RF window and to act as an RF shielding element for the RF ion source. When the heating/RF shielding element is in a heating mode, it suppresses formation of unwanted deposits on the RF window which negatively impacts the transfer of RF energy from an RF antenna to a plasma chamber. When the heating/RF-shielding element is in a shielding mode, it provides an electrostatic shielding for the RF ion source.

Abstract: Disclosed is an inductively coupled RF plasma source that provides both magnetic confinement to reduce plasma losses and Faraday shielding to suppress parasitic capacitive components. The inductively coupled RF plasma system comprises an RF power source, plasma chamber, an array of permanent magnets, and an antenna array. The plasma chamber is comprised of walls and a dielectric window having an inner and outer surface wherein the inner surface forms a wall of the plasma chamber. The array of parallel conductive permanent magnets is electrically interconnected and embedded within the dielectric window walls proximate to the inner surface and coupled to ground on one end. The permanent magnet array elements are alternately magnetized toward and away from plasma in the plasma chamber to form a multi-cusp magnetic field. The antenna array may be comprised of parallel tubes through which an RF current is circulated. The antenna array is oriented perpendicular to the permanent magnet array.

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.

Abstract: An ion source, capable of generating high density wide ribbon ion beam, utilizing one or more helicon plasma sources is disclosed. In addition to the helicon plasma source(s), the ion source also includes a diffusion chamber. The diffusion chamber has an extraction aperture oriented along the same axis as the dielectric cylinder of the helicon plasma source. In one embodiment, dual helicon plasma sources, located on opposing ends of the diffusion chamber are used to create a more uniform extracted ion beam. In a further embodiment, a multicusp magnetic field is used to further improve the uniformity of the extracted ion beam.

Abstract: An ion source, capable of generating high-density wide ribbon ion beam, utilizing inductively coupled plasma production is disclosed. As opposed to conventional ICP sources, the present disclosure describes an ICP source which is not cylindrical. Rather, the source is defined such that its width, which is the dimension along which the beam is extracted, is greater than its height. The depth of the source may be defined to maximize energy transfer from the antenna to the plasma. In a further embodiment, a multicusp magnetic field surrounding the ICP source is used to further increase the current density and improve the uniformity of the extracted ion beam. Ion beam uniformity can also be controlled by means of several independent controls, including gas flow rate, and input RF power.

Abstract: An RF ion source utilizing a heating/RF-shielding element for controlling the temperature of an RF window and to act as an RF shielding element for the RF ion source. When the heating/RF shielding element is in a heating mode, it suppresses formation of unwanted deposits on the RF window which negatively impacts the transfer of RF energy from an RF antenna to a plasma chamber. When the heating/RF-shielding element is in a shielding mode, it provides an electrostatic shielding for the RF ion source.

Abstract: An ion source, capable of generating high-density wide ribbon ion beam, utilizing one or more plasma sources is disclosed. In addition to the plasma source(s), the ion source also includes a diffusion chamber. The diffusion chamber has an extraction aperture oriented along the same axis as the dielectric cylinder of the plasma source. In one embodiment, dual plasma sources, located on opposing ends of the diffusion chamber are used to create a more uniform extracted ion beam. In a further embodiment, a multicusp magnetic field is used to further improve the uniformity of the extracted ion beam.