Abstract:
The present invention is a method to enhance accuracy of irradiation with beam for an irradiation system with a beam. The irradiation system comprises a beam generation source, a mass analysis device, a beam transformer, a scanner which swings the beam reciprocally with high speed, a beam parallelizing device, an acceleration/deceleration device, an energy filtering device, and beam monitors. The beam transformer comprises a vertically focusing synchronized quadrupole electromagnet syQD and a horizontally focusing synchronized quadrupole electromagnet syQF. Consequently, it is possible to correct at least one of a deviation in beam divergence angle and a deviation in beam size within a range between a center trajectory and an outer trajectory after swinging of the beam by the scanner.
Abstract:
Various aspects of the invention provide improved approaches and methods for efficiently: Vaporizing decaborane and other heat-sensitive materials via a novel vaporizer and vapor delivery system; Delivering a controlled, low-pressure drop flow of vapors, e.g. decaborane, into the ion source; Ionizing the decaborane into a large faction of B10Hx+; Preventing thermal dissociation of decaborane; Limiting charge-exchange and low energy electron-induced fragmentation of B10Hx+; Operating the ion source without an arc plasma, which can improve the emittance properties and the purity of the beam; Operating the ion source without use of a strong applied magnetic field, which can improve the emittance properties of the beam; Using a novel approach to produce electron impact ionizations without the use of an arc discharge, by incorporation of an externally generated, broad directional electron beam which is aligned to pass through the ionization chamber to a thermally isolated beam dump; Providing production-worthy dosage rates of boron dopant at the wafer; Providing a hardware design that enables use also with other dopants, especially using novel hydride, dimer-containing, and indium- or antimony-containing temperature-sensitive starting materials, to further enhance the economics of use and production worthiness of the novel source design and in many cases, reducing the presence of contaminants; Matching the ion optics requirements of the installed base of ion implanters in the field; Eliminating the ion source as a source of transition metals contamination, by using an external and preferably remote cathode and providing an ionization chamber and extraction aperture fabricated of non-contaminating material, e.g. graphite, silicon carbide or aluminum; Enabling retrofit of the new ion source into the ion source design space of existing Bernas source-based ion implanters and the like or otherwise enabling compatibility with other ion source designs; Using a control system in retrofit installations that enables retention of the installed operator interface and control techniques with which operators are already familiar; Enabling convenient handling and replenishment of the solid within the vaporizer without substantial down-time of the implanter; Providing internal adjustment and control techniques that enable, with a single design, matching the dimensions and intensity of the zone in which ionization occurs to the beam line of the implanter and the requirement of the process at hand; Providing novel approaches, starting materials and conditions of operation that enable the making of future generations of semiconductor devices and especially CMOS source/drains and extensions, and doping of silicon gates.
Abstract:
Various aspects of the invention provide improved approaches and methods for efficiently: Vaporizing decaborane and other heat-sensitive materials via a novel vaporizer and vapor delivery system; Delivering a controlled, low-pressure drop flow of vapors, e.g. decaborane, into the ion source; Ionizing the decaborane into a large fraction of B10Hxnull; Preventing thermal dissociation of decaborane; Limiting charge-exchange and low energy electron-induced fragmentation of B10Hxnull; Operating the ion source without an arc plasma, which can improve the emittance properties and the purity of the beam; Operating the ion source without use of a strong applied magnetic field, which can improve the emittance properties of the beam; Using a novel approach to produce electron impact ionizations without the use of an arc discharge, by incorporation of an externally generated, broad directional electron beam which is aligned to pass through the ionization chamber to a thermally isolated beam dump; Providing production-worthy dosage rates of boron dopant at the wafer; Providing a hardware design that enables use also with other dopants, especially using novel hydride, dimer-containing, and indium- or antimony-containing temperature-sensitive starting materials, to further enhance the economics of use and production worthiness of the novel source design and in many cases, reducing the presence of contaminants; Matching the ion optics requirements of the installed base of ion implanters in the field; Eliminating the ion source as a source of transition metals contamination, by using an external and preferably remote cathode and providing an ionization chamber and extraction aperture fabricated of non-contaminating material, e.g. graphite, silicon carbide or aluminum; Enabling retrofit of the new ion source into the ion source design space of existing Bernas source-based ion implanters and the like or otherwise enabling compatibility with other ion source designs; Using a control system in retrofit installations that enables retention of the installed operator interface and control techniques with which operators are already familiar; Enabling convenient handling and replenishment of the solid within the vaporizer without substantial down-time of the implanter; Providing internal adjustment and control techniques that enable, with a single design, matching the dimensions and intensity of the zone in which ionization occurs to the beam line of the implanter and the requirement of the process at hand; Providing novel approaches, starting materials and conditions of operation that enable the making of future generations of semiconductor devices and especially CMOS source/drains and extensions, and doping of silicon gates.
Abstract:
An ion source is disclosed having an elongated slit for providing a ribbon ion beam for use in an ion implantation system. The source comprises a coaxial inductive coupling antenna for RF excitation of plasma within a cylindrical source housing, as well as circumferential magnets disposed within the housing for generating azimuthal multi-cusped magnetic fields for plasma confinement. Also disclosed is a liner for the housing interior providing thermal barrier between the plasma and the outer housing wall so as to mitigate or reduce condensation within the plasma confinement chamber.
Abstract:
An ion source is disclosed for ion implantation applications, having control apparatus for selectively adjusting a density profile associated with an elongated ion beam being extracted from a plasma confinement chamber. The control apparatus comprises a plurality of magnet pairs proximate an elongated extraction exit through which a ribbon beam is extracted from the ion source, with the magnet pairs individually comprising upper and lower electro-magnets disposed above and below the extraction exit opening to provide adjustable magnetic fields in a pre-extraction region so as to adjust the density profile of an extracted ribbon beam.
Abstract:
Ion implantation systems and beamlines therefor are disclosed, in which a ribbon beam of a relatively large aspect ratio is mass analyzed and collimated to provide a mass analyzed ribbon beam for use in implanting one or more workpieces. The beamline system comprises two similar magnets, where the first magnet mass analyzes the ribbon beam to provide an intermediate mass analyzed ion beam, and the second magnet collimates the intermediate beam to provide a uniform mass analyzed ribbon beam to an end station. The symmetrical system provides equidistant beam trajectories for ions across the elongated beam width so as to mitigate non-linearities in the beam transport through the system, such that the resultant mass analyzed beam is highly uniform.
Abstract:
Provided is a charged particle beam applied apparatus for observing a sample, provided with: a beam-forming section that forms a plurality of charged particle beams on a sample; an energy control unit that controls the incident energy of the plurality of charged particle beams that are irradiated onto the sample; a beam current control unit that controls the beam current of the plurality of charged particle beams that are irradiated onto the sample; and a beam arrangement control unit that controls the arrangement in which the plurality of charged particle beams is irradiated onto the sample. The beam-forming section includes a beam splitting electrode, a lens array upper electrode, a lens array middle electrode, a lens array lower electrode and a movable stage, and functions as the beam current control unit or the beam arrangement control unit through selection, by the movable stage, of a plurality of aperture pattern sets.
Abstract:
Provided is a charged particle beam applied apparatus for observing a sample, provided with: a beam-forming section that forms a plurality of charged particle beams on a sample; an energy control unit that controls the incident energy of the plurality of charged particle beams that are irradiated onto the sample; a beam current control unit that controls the beam current of the plurality of charged particle beams that are irradiated onto the sample; and a beam arrangement control unit that controls the arrangement in which the plurality of charged particle beams is irradiated onto the sample. The beam-forming section includes a beam splitting electrode, a lens array upper electrode, a lens array middle electrode, a lens array lower electrode and a movable stage, and functions as the beam current control unit or the beam arrangement control unit through selection, by the movable stage, of a plurality of aperture pattern sets.
Abstract:
An ion source is disclosed for use in fabrication of semiconductors. The ion source includes an electron emitter that includes a cathode mounted external to the ionization chamber for use in fabrication of semiconductors. In accordance with an important aspect of the invention, the electron emitter is employed without a corresponding anode or electron optics. As such, the distance between the cathode and the ionization chamber can be shortened to enable the ion source to be operated in an arc discharge mode or generate a plasma. Alternatively, the ion source can be operated in a dual mode with a single electron emitter by selectively varying the distance between the cathode and the ionization chamber.
Abstract:
A novel technique is disclosed for varying a size of an aperture within a vacuum chamber. A drive mechanism within the vacuum chamber is used to adjust a partial horizontal overlap between at least two blades, wherein a perimeter of the aperture opening is defined by edges of said blades. In one embodiment, a variable aperture mechanism includes first and second blades attached to a first support, and third and fourth blades attached to a second support. The first blade is spaced vertically above the second blade on the first support; a second support, and the fourth blade is spaced vertically above the third blade on the second support. There is a partial horizontal overlap between the first and third blades and between the fourth and second blades, and the aperture opening has a perimeter defined by edges of the four blades. Other embodiments are also disclosed.