Abstract:
PROBLEM TO BE SOLVED: To provide an electrical insulator tetrode lens assembly preventing insulation breakdown caused by voltage. SOLUTION: The electrostatic tetrode lens assembly 60 comprises four electrodes, namely, a first electrode pair 84a, 84c each of which is laid out from the axial line 86 to the outside of the radial direction approximately 90 deg. apart and located at the opposite sides 180 deg. apart and a second electrode pair 84b, 84d located at opposite sides 180 deg. apart, the housing 62 equipped with the installation surface 64 to install the electrostatic tetrode lens assembly 60 on the ion injection device, the first and the second electric leads 104, 108 to supply power to the above No.1 and No.2 electrode pairs 104, 108, and a plural number of electric insulation members 92 made of a glass material including the first, the second electric insulation members to mount the first, the second electrode pairs on the housing. The insulation materials have a resistance to the accumulated graphite scattered from the electrodes and diminish breakdown by a high voltage/current.
Abstract:
An integrated RF amplifier and resonator is provided for use with an ion accelerator. The amplifier includes an output substantially directly coupled with a resonator coil. The amplifier output may be coupled capacitively or inductively. In addition, an apparatus is provided for accelerating ions in an ion implanter. The apparatus comprises an amplifier with an RF output, a tank circuit with a coil substantially directly coupled to the RF output of the amplifier, and an electrode connected to the coil for accelerating ions. Also provided is a method for coupling an RF amplifier with a resonator in an ion accelerator. The method comprises connecting the RF output of the amplifier to a coupler, and locating the coupler proximate the coil, thereby substantially directly coupling the RF output of the amplifier with the resonator coil.
Abstract:
A mass analysis magnet assembly (16) is provided for use in an ion implanter (10), comprising: (i) a magnet (44) for mass analyzing an ion beam (15) output by an ion source (14), the magnet providing an interior region (49) through which the ion beam passes; and (ii) a neutron containment chamber (52) coupled to the magnet (44). The neutron containment chamber provides a containment space (58) in communication with the interior region (49) of the magnet (44), and a neutron absorbing wall (54) that in part defines the containment space. The neutron-absobing wall (54) is at least partially covered by a lining (56) capable of releasing neutrons when impacted by deuterons that are carried along with the ion beam (15) through the containment space (58). Preferably, the linning (56) is comprised of graphite, and the wall is comprised of either paraffin or polyethylene. The wall (54) includes portions (60) that either absorb neutrons released by the graphite lining (56) or substantially reduce the energies thereof.
Abstract:
An integrated RF amplifier (120) and resonator (100) is provided for use with an ion accelerator. The amplifier (120) includes an output substantially directly coupled with a resonator coil (L). The amplifier output may be coupled capacitively or inductively. In addition, an apparatus is provided for accelerating ions in an ion implanter. The apparatus comprises an amplifier (120) with an RF output (122), a tank circuit (100) with a coil (L) substantially directly coupled to the RF output (122) of the amplifier (120), and an electrode (108) connected to the coil (L) for accelerating ions. Also provided is a method (500) for coupling an RF amplifier (120) with a resonator (100) in an ion accelerator. The method comprises connecting (502) the RF output (122) of the amplifier (120) to a coupler, and locating (504) the coupler proximate the coil (L), thereby substantially directly coupling the RF output (122) of the amplifier (120) with the resonator coil (L).
Abstract:
An ion buncher stage for a linear accelerator system is disclosed for bunching ions in an ion implantation system. The ion buncher stage may be employed upstream of one or more accelerating stages such that the loss of ions in the linear accelerator system is reduced. The invention further includes an asymmetrical double gap buncher stage, as well as a slit buncher stage for further improvement of ion implantation efficiency. Also disclosed are methods for accelerating ions in an ion implanter linear accelerator.
Abstract:
A method and apparatus are disclosed for accelerating ions in an ion implantation system. An ion accelerator is provided which comprises a plurality of energizable electrodes energized by a variable frequency power source, in order to accelerate ions from an ion source. The variable frequency power source allows the ion accelerator to be adapted to accelerate a wide range of ion species to desired energy levels for implantation onto a workpiece, while reducing the cost and size of an ion implantation accelerator.
Abstract:
In accordance with the present invention, an ion implanter (10) including a time of flight energy measurement apparatus (200) for measuring and controlling the energy of an ion beam (14). The ion implanter (10) includes an ion source (12) for generating the ion beam (14), an ion acceleration assembly (18) for accelerating the beam (14) resulting in the beam (14) comprising a series of ion pulses (P0, P1, ...., P(n+1)) having a predetermined frequency (F) and beam forming and directing structure (50) for directing the ion beam (14) at workpieces (21) supported in an implantation chamber (22) of the implanter (10). The time of flight energy measurement apparatus (200) includes spaced apart first and second sensors (210, 310, 220, 320), timing circuitry (204) and conversion circuitry (206). The time of flight energy measurement apparatus (200) measures an average kinetic energy of an ion (E(ion)) included in a selected ion pulse of the ion beam. The first sensor (210, 310) and a second sensor (220, 320) are disposed adjacent the ion beam (14) and spaced a predetermined distance apart, the second sensor (220, 320) being downstream of the first sensor (210, 310). The first sensor (210, 310) generates a signal when an ion pulse of the ion beam (14) passes the first sensor (210, 310) and the second sensor (220, 320) generates a signal when an ion pulse of the ion beam (14) passes the second sensor (220, 320). The timing circuitry (204) of the energy measurement apparatus (200) is electrically coupled to the first and second sensors (210, 310, 220, 320) and determines an elapsed time, t, for the selected ion pulse to traverse the predetermined distance between the first and second sensors (210, 310, 220, 320). The timing circuitry (204) calculates an average number of ion pulses. N. in the ion beam (14) between the first and second sensors (210, 310, 220, 320) based on the approximation of the ion beam energy (E(approx.)) and calculates an offset time. t(offset). for the selected ion pulse using the formula, t(offset) = N x T. The timing circuitry (204) than determines the elapsed time, t. The conversion circuitry (206) converts the elapsed time. t. for the selected ion pulse into a measure of the energy of the ion beam (E(ion)).
Abstract:
An integrated RF amplifier (120) and resonator (100) is provided for use with an ion accelerator. The amplifier (120) includes an output substantially directly coupled with a resonator coil (L). The amplifier output may be coupled capacitively or inductively. In addition, an apparatus is provided for accelerating ions in an ion implanter. The apparatus comprises an amplifier (120) with an RF output (122), a tank circuit (100) with a coil (L) substantially directly coupled to the RF output (122) of the amplifier (120), and an electrode (108) connected to the coil (L) for accelerating ions. Also provided is a method (500) for coupling an RF amplifier (120) with a resonator (100) in an ion accelerator. The method comprises connecting (502) the RF output (122) of the amplifier (120) to a coupler, and locating (504) the coupler proximate the coil (L), thereby substantially directly coupling the RF output (122) of the amplifier (120) with the resonator coil (L).
Abstract:
A mass analysis magnet assembly (16) is provided for use in an ion implanter (10), comprising: (i) a magnet (44) for mass analyzing an ion beam (15) output by an ion source (14), the magnet providing an interior region (49) through which the ion beam passes; and (ii) a neutron containment chamber (52) coupled to the magnet (44). The neutron containment chamber provides a containment space (58) in communication with the interior region (49) of the magnet (44), and a neutron absorbing wall (54) that in part defines the containment space. The neutron-absobing wall (54) is at least partially covered by a lining (56) capable of releasing neutrons when impacted by deuterons that are carried along with the ion beam (15) through the containment space (58). Preferably, the linning (56) is comprised of graphite, and the wall is comprised of either paraffin or polyethylene. The wall (54) includes portions (60) that either absorb neutrons released by the graphite lining (56) or substantially reduce the energies thereof.
Abstract:
A mass analysis magnet assembly (16) is provided for use in an ion implanter (10), comprising: (i) a magnet (44) for mass analyzing an ion beam (15) output by an ion source (14), the magnet providing an interior region (49) through which the ion beam passes; and (ii) at least one strike plate (48) in part forming an outer boundary of the interior region (49). The at least one strike plate is comprised of an isotopically pure carbon-based material. The isotopically pure carbon-based material, preferably by mass greater than 99 % carbon C-12, prevents neutron radiation when impacted by deuterons extracted from the ion source (14). The strike plate (48) may comprise an upper layer (56) of isotopically pure carbon C-12 isotope positioned atop a lower substrate (54).