Abstract:
An ion source for use in a radiation generator tube includes a back passive cathode electrode, a passive anode electrode downstream of the back passive cathode electrode, a magnet adjacent the anode, and a front passive cathode electrode downstream of the passive anode electrode. The front passive cathode electrode and the back passive cathode electrode define an ionization region therebetween. At least one field emitter array (FEA) cathode is configured to electrostatically discharge due to an electric field in the ion source. The back passive cathode electrode and the passive anode electrode, and the front passive cathode electrode and the passive anode electrode, have respective voltage differences therebetween, and the magnet generating a magnetic field, such that a Penning-type trap is produced to confine electrons from the electrostatic discharge to the ionization region. At least some of the electrons in the ionization region interact with an ionizable gas to create ions.
Abstract:
A method of controlling operation of an indirectly-heated cathode (IHC) ion source includes a step of measuring a rate of loss of cathode weight of the IHC ion source that occurs during operation using a first cathode configuration and under a first set of operation conditions. A maximum weight loss for the first cathode configuration is determined, and a cathode lifetime is calculated based upon the rate of cathode weight loss and the maximum weight loss. A further method includes receiving a minimum source bias power value for operation of a cathode in a first configuration, measuring a rate of decrease in source bias power for a cathode in the first configuration, and calculating a lifetime of the cathode based upon the minimum source bias power and rate of decrease in source bias power.
Abstract:
A plasma is formed from one or more gases in a plasma chamber using at least a first power and a second power. A first ion species is generated at said first power and a second ion species is generated at said second power. In one embodiment, the first ion species and second ion species are implanted into a workpiece at two different energies using at least a first bias voltage and a second bias voltage. This may enable implantation to two different depths. These ion species may be atomic ions or molecular ions. The molecular ions may be larger than the gases used to form the plasma.
Abstract:
A focused ion beam (FIB) system is disclosed, comprising an inductively coupled plasma ion source, an insulating plasma chamber containing the plasma, a conducting source biasing electrode in contact with the plasma and biased to a high voltage to control the ion beam energy at a sample, and a plurality of apertures. The plasma within the plasma chamber serves as a virtual source for an ion column comprising one or more lenses which form a focused ion beam on the surface of a sample to be imaged and/or FIB-processed. The plasma is initiated by a plasma igniter mounted near or at the column which induces a high voltage oscillatory pulse on the source biasing electrode. By mounting the plasma igniter near the column, capacitive effects of the cable connecting the source biasing electrode to the biasing power supply are minimized. Ion beam sputtering of the apertures is minimized by proper aperture materials selection.
Abstract:
A method of manufacturing a semiconductor device is described. The method comprises performing a gas cluster ion beam (GCIB) pre-treatment and/or post-treatment of at least a portion of a silicon-containing substrate during formation of a silicide region.
Abstract:
According to one embodiment, a manufacturing method of a magnetoresistive effect element includes forming a laminated structure on a substrate, the laminated structure including a first magnetic layer having a variable magnetization direction, a second magnetic layer having an invariable magnetization direction, and a non-magnetic layer between the first and second magnetic layers, forming a first mask layer having a predetermined plane shape on the laminated structure, and processing the laminated structure based on the first mask layer by using an ion beam whose solid angle in a center of the substrate is 10° or more.
Abstract:
A system and method of treating air. Bipolar ionization is delivered to an airflow within a conduit from a tubeless ion generator. The ionized airflow may be delivered to a conditioned airspace by an HVAC system. In alternate applications, the airflow delivers ionized combustion air to an engine. The invention also includes a mounting assembly for positioning one or more ion generators into an airflow.
Abstract:
A system for improving ion beam quality is disclosed. According to one embodiment, the system comprises an ion source, having a chamber defined by a plurality of chamber walls; an RF antenna disposed on a first wall of the plurality of chamber walls; a second wall, opposite the first wall, the distance between the first wall and the second wall defining the height of the chamber; an aperture disposed on one of the plurality of chamber walls; a first gas inlet for introducing a first source gas to the chamber; and a second gas inlet for introducing a second source gas, different from the first source gas, to the chamber; wherein a first distance from the first gas inlet to the second wall is less than 35% of the height; and a second distance from the second gas inlet to the first wall is less than 35% of the height.
Abstract:
An ion generation method uses a direct current discharge ion source provided with an arc chamber formed of a high melting point material, and includes: generating ions by causing molecules of a source gas to collide with thermoelectrons in the arc chamber and producing plasma discharge; and causing radicals generated in generating ions to react with a liner provided to cover an inner wall of the arc chamber at least partially. The liner is formed of a material more reactive to radicals generated as the source gas is dissociated than the material of the arc chamber.
Abstract:
A method of manufacturing a semiconductor device includes the steps of: providing a supply of molecules containing a plurality of dopant atoms into an ionization chamber, ionizing said molecules into dopant cluster ions, extracting and accelerating the dopant cluster ions with an electric field, selecting the desired cluster ions by mass analysis, modifying the final implant energy of the cluster ion through post-analysis ion optics, and implanting the dopant cluster ions into a semiconductor substrate. In general, dopant molecules contain n dopant atoms, where n is an integer number greater than 10. This method enables increasing the dopant dose rate to n times the implantation current with an equivalent per dopant atom energy of 1/n times the cluster implantation energy, while reducing the charge per dopant atom by the factor n.