Abstract: Thermal control is provided for an extraction electrode of an ion-beam producing system that prevents formation of deposits and unstable operation and enables use with ions produced from condensable vapors and with ion sources capable of cold and hot operation. Electrical heating of the extraction electrode is employed for extracting decaborane or octadecaborane ions. Active cooling during use with a hot ion source prevents electrode destruction, permitting the extraction electrode to be of heat-conductive and fluorine-resistant aluminum composition.

Abstract: The service lifetime of an ion source is enhanced or prolonged by the source having provisions for in-situ etch cleaning of the ion source and of an extraction electrode, using reactive halogen gases (F or Cl), and by having features that extend the service duration between cleanings. The latter include accurate vapor flow control, accurate focusing of the ion beam optics, and thermal control of the extraction electrode that prevents formation of deposits or prevents electrode destruction. An apparatus comprised of an ion source for generating dopant ions for semiconductor wafer processing is coupled to a remote plasma source which delivers F or Cl ions to the first ion source for the purpose of cleaning deposits in the first ion source and the extraction electrode. These methods and apparatus enable long equipment uptime when running condensable feed gases such as sublimated vapor sources, and are particularly applicable for use with so-called cold ion sources.

Abstract: Thermal control is provided for an extraction electrode of an ion-beam producing system that prevents formation of deposits and unstable operation and enables use with ions produced from condensable vapors and with ion sources capable of cold and hot operation. Electrical heating of the extraction electrode is employed for extracting decaborane or octadecaborane ions. Active cooling during use with a hot ion source prevents electrode destruction, permitting the extraction electrode to be of heat-conductive and fluorine-resistant aluminum composition. The service lifetime of the system is enhanced by provisions for in-situ etch cleaning of the ion source and extraction electrode, using reactive halogen gases, and by having features that extend the service duration between cleanings, including accurate vapor flow control and accurate focusing of the ion beam optics.

Abstract: Thermal control is provided for an extraction electrode of an ion-beam producing system that prevents formation of deposits and unstable operation and enables use with ions produced from condensable vapors and with ion sources capable of cold and hot operation. Electrical heating of the extraction electrode is employed for extracting decaborane or octadecaborane ions. Active cooling during use with a hot ion source prevents electrode destruction, permitting the extraction electrode to be of heat-conductive and fluorine-resistant aluminum composition. The service lifetime of the system is enhanced by provisions for in-situ etch cleaning of the ion source and extraction electrode, using reactive halogen gases, and by having features that extend the service duration between cleanings, including accurate vapor flow control and accurate focusing of the ion beam optics.

Abstract: The service lifetime of an ion source is enhanced or prolonged by the source having provisions for in-situ etch cleaning of the ion source and of an extraction electrode, using reactive halogen gases, and by having features that extend the service duration between cleanings. The latter include accurate vapor flow control, accurate focusing of the ion beam optics, and thermal control of the extraction electrode that prevents formation of deposits or prevents electrode destruction. An apparatus comprised of an ion source for generating dopant ions for semiconductor wafer processing is coupled to a remote plasma source which delivers F or Cl ions to the first ion source for the purpose of cleaning deposits in the first ion source and the extraction electrode. These methods and apparatus enable long equipment uptime when running condensable feed gases such as sublimated vapor sources, and are particularly applicable for use with so-called cold ion sources.

Abstract: Ion implantation with high brightness, ion beam by ionizing gas or vapor, e.g. of dimers, or decaborane, by direct electron impact ionization adjacent the outlet aperture (46, 176) of the ionization chamber (80; 175)). Preferably: conditions are maintained that produce a substantial ion density and limit the transverse kinetic energy of the ions to less than 0.7 eV; width of the ionization volume adjacent the aperture is limited to width less than about three times the width of the aperture; the aperture is extremely elongated; magnetic fields are avoided or limited; low ion beam noise is maintained; conditions within the ionization chamber are maintained that prevent formation of an arc discharge. With ion beam optics, such as the batch implanter of FIG. (20), or in serial implanters, ions from the ion source are transported to a target surface and implanted; advantageously, in some cases, in conjunction with acceleration-deceleration beam lines employing cluster ion beams.

Abstract: An ion implantation is disclosed that includes an ionization chamber having a restricted outlet aperture and configured so that the gas or vapor in the ionization chamber is at a pressure substantially higher than the pressure within an extraction region into which the ions are to be extracted external to the ionization chamber. The vapor is ionized by direct electron impact ionization by an electron source that is in a region adjacent the outlet aperture of the ionization chamber to produce ions from the molecules of the gas or vapor to a density of at least 1010 cm?3 at the aperture while maintaining conditions that limit the transverse kinetic energy of the ions to less than about 0.7 eV. The beam is transported to a target surface and the ions of the transported ion beam are implanted into the target.

Abstract: An ion implantation is disclosed that includes an ionization chamber having a restricted outlet aperture and configured so that the gas or vapor in the ionization chamber is at a pressure substantially higher than the pressure within an extraction region into which the ions are to be extracted external to the ionization chamber. The vapor is ionized by direct electron impact ionization by an electron source that is in a region adjacent the outlet aperture of the ionization chamber to produce ions from the molecules of the gas or vapor to a density of at least 1010 cm?3 at the aperture while maintaining conditions that limit the transverse kinetic energy of the ions to less than about 0.7 eV. The beam is transported to a target surface and the ions of the transported ion beam are implanted into the target.

Abstract: Ion implantation with high brightness, ion beam by ionizing gas or vapor, e.g. of dimers, or decaborane, by direct electron impact ionization adjacent the outlet aperture (46, 176) of the ionization chamber (80; 175)). Preferably: conditions are maintained that produce a substantial ion density and limit the transverse kinetic energy of the ions to less than 0.7 eV; width of the ionization volume adjacent the aperture is limited to width less than about three times the width of the aperture; the aperture is extremely elongated; magnetic fields are avoided or limited; low ion beam noise is maintained; conditions within the ionization chamber are maintained that prevent formation of an arc discharge. With ion beam optics, such as the batch implanter of FIG. (20), or in serial implanters, ions from the ion source are transported to a target surface and implanted; advantageously, in some cases, in conjunction with acceleration-deceleration beam lines employing cluster ion beams.

Abstract: Ion implantation with high brightness, ion beam by ionizing gas or vapor, e.g. of dimers, or decaborane, by direct electron impact ionization adjacent the outlet aperture (46, 176) of the ionization chamber (80; 175)). Preferably: conditions are maintained that produce a substantial ion density and limit the transverse kinetic energy of the ions to less than 0.7 eV; width of the ionization volume adjacent the aperture is limited to width less than about three times the width of the aperture; the aperture is extremely elongated; magnetic fields are avoided or limited; low ion beam noise is maintained; conditions within the ionization chamber are maintained that prevent formation of an arc discharge. With ion beam optics, such as the batch implanter of FIG. (20), or in serial implanters, ions from the ion source are transported to a target surface and implanted; advantageously, in some cases, in conjunction with acceleration-deceleration beam lines employing cluster ion beams.

Abstract: A high temperature gas stream optical flame sensor for flame detection in gas turbine engines, the sensor generally comprising a silicon carbide photodiode and silicon carbide based amplification hardware for generating a signal indicative of the presence of the flame, in some embodiments the photodiode and amplification hardware being disposed within a sensor housing, in another embodiment for use in an aeroderivative premixed combustion system, the photodiode being situated within a fuel/air premixer.