Abstract:
An elevated temperature RF ion source system, comprising an ion source body, an RF antenna coil external to the ion source body, a vacuum enclosure surrounding both the outside surface of the ion source body and the RF antenna coil, at least one power supply, a gas delivery system operatively coupled to the ion source body, a vacuum condition between the outside surface of the ion source body and the RF antenna coil, the RF antenna coil operatively coupled to the at least one power supply, and a water cooling system operatively coupled to the RF antenna coil and the vacuum enclosure.
Abstract:
An ion doping apparatus includes: a chamber 11; a discharge section 13 for discharging a gaseous content from within the chamber 11; an ion source 12 being provided in the chamber 11 and including an inlet 14 through which to introduce a gas containing an element to be used for doping, the ion source 12 decomposing the gas introduced through the inlet 14 to generate ions containing the element to be used for doping; an acceleration section 23 for pulling out from the ion source 12 the ions generated at the ion source 12 and accelerating the ions toward a target object held in the chamber; and a beam current meter 26 for measuring a beam current caused by the accelerated ions. The beam current is measured by the beam current meter 26 a plurality of times, and if a result of the measurements indicates a stability of the beam current, the ion doping apparatus automatically begins to implant into the target object the ions containing the element to be used for doping. Thus, an ion doping apparatus having excellent doping amount controllability is provided.
Abstract:
An ion source that utilizes exited and/or atomic gas injection is disclosed. In an ion beam application, the source gas can be used directly, as it is traditionally supplied. Alternatively or additionally, the source gas can be altered by passing it through a remote plasma source prior to being introduced to the ion source chamber. This can be used to create excited neutrals, heavy ions, metastable molecules or multiply charged ions. In another embodiment, multiple gasses are used, where one or more of the gasses are passed through a remote plasma generator. In certain embodiments, the gasses are combined in a single plasma generator before being supplied to the ion source chamber. In plasma immersion applications, plasma is injected into the process chamber through one or more additional gas injection locations. These injection locations allow the influx of additional plasma, produced by remote plasma sources external to the process chamber.
Abstract:
An ion source is disclosed that is capable of providing ions of decaborane in commercial ion current levels to the ion extraction system of an ion implanter is provided, the ion source comprising an ionization chamber defined by walls enclosing an ionization volume, there being an ion extraction aperture in a side wall of the ionization chamber, arranged to enable the ion current to be extracted from the ionization volume by an extraction system, an electron gun mounted on a support that is outside of and thermally isolated from the walls of the ionization chamber, the ion extraction aperture plate is biased to a negative voltage with respect to the ionization chamber to further increase the drift velocity of the ions, and hence the maximum obtainable current in the resulting ion beam.
Abstract:
Disclosed herein are apparatus and methods for selectively depositing molecular ions on nanoscale substrates such as carbon nanotube arrays using electrospray ionization.
Abstract:
A spin polarized ion beam generation apparatus (30) can efficiently generate a spin polarized ion by using a pumping light generator (33) to an ion in a high frequency discharge tube (15) to irradiate optical pumping (33,34) by circularly polarized light and linearly polarized light orthogonal to each other to a metastable atom. For example, a polarized helium ion beam having a spin polarization rate that exceeds 18% and that is as high as 25% can be generated. The spin polarized ion beam generation apparatus (30) also can be applied to a processing apparatus and an analysis apparatus that can irradiate a polarized ion beam to a specimen. According to the spin polarized ion scattering spectroscopy apparatus, the spin status in a region at a depth of about 2 to 3 atomic layers from the surface of the specimen can be measured while discriminating the elements from the atomic layer with a reduced measurement time and with a high accuracy impossible in the conventional technique.
Abstract:
A capillaritron ion beam sputtering system and a thin film production method are disclosed. By utilizing reactive capillaritron ion beam sputtering deposition, argon and oxygen are passed through a capillaritron ion source simultaneously. Argon is being ionized and accelerated by a voltage to bombard a zinc target and create zinc atoms, while oxygen atoms are created at the same time. Zinc atom and oxygen atom are combined to form ZnO to deposit on a substrate. The stoichiometric properties, deposition rate, transmission properties, surface roughness and film density of the as-deposited film can be altered by adjusting capillaritron ion beam energy and oxygen partial pressure. Using preferred processing parameters, the root-mean-square surface roughness of the as-deposited film can be smaller than 1.5 nm, while the transmission coefficient at visible range can be greater than 80%.
Abstract:
A multicharged ions generating source that is easy to manufacture, excellent in controllability and maintainability, high in degree of ionization and large in beam intensity and a charged particle beam apparatus using the same are disclosed. The multicharged ions generating source includes an ion source electrode (3) comprising an electron source (4), a drift tube (5) that constitutes an ion trapping region and a collector (6), a superconducting magnet (11) for ion entrapment, an ion infeed means (20, 22), a first vacuum chamber (2) receiving the ion source electrode (3), a second vacuum chamber (10) receiving the superconducting magnet (11), and a vacuum pumping unit (15, 16) provided for each of the first and second vacuum chambers. The first and the second vacuum chambers (2) and (10) are made removable from each other, and only the ion source electrode (3) to be held at extremely high vacuum can be baked for degassing.
Abstract:
An apparatus for producing negative ions including an emitter coated with an ionic liquid room-temperature molten salt, an electrode positioned downstream relative to the emitter, a power supply that applies a voltage to the emitter with respect to the electrode. The power supply is sufficient to generate a stable high brightness beam of negative ions having minimal chromatic and spherical aberrations in the beam. An electrostatic lens and deflector is used to focus and direct the beam to a target.
Abstract:
An ion source is provided that can generate an ion beam in which the width is wide, the beam current is large, and the uniformity of the beam current distribution in the width direction is high, and that can prolong the lifetime of a cathode.The ion source 2a has: a plasma generating chamber 6 having an ion extraction port 8 extending in the X direction; a magnet 14 which generates a magnetic field 16 extending along the X direction, in the plasma generating chamber 6; indirectly-heated cathodes 20 which are placed respectively on the both sides of the plasma generating chamber 6 in the X direction, and which are used for generating a plasma 10 in the chamber 6, and increasing or decreasing the density of the whole of the plasma 10; and plural filament cathodes 32 which are juxtaposed in the X direction in the plasma generating chamber 6, and which are used for generating the plasma 10 in the chamber 6, and controlling the density distribution of the plasma 10.