An apparatus for the creation of high current ion beams is disclosed. The apparatus includes an ion source, such as a RF ion source or an indirectly heated cathode (IHC) ion source, having an extraction aperture. Disposed proximate the extraction aperture is a bias electrode, which has a hollow center portion that is aligned with the extraction aperture. A magnetic field is created along the perimeter of the hollow center portion, which serves to contain electrons within a confinement region. Electrons in the confinement region energetically collide with neutral particles, increasing the number of ions that are created near the extraction aperture. The magnetic field may be created using two magnets that are embedded in the bias electrode. Alternatively, a single magnet or magnetic coils may be used to create this magnetic field.

A soft-landing (SL) instrument for depositing ions onto substrates using a laser ablation source is described herein. The instrument of the instant invention is designed with a custom drift tube and a split-ring ion optic for the isolation of selected ions and is capable of operating at atmospheric pressure. The drift tube allows for the separation and thermalization of ions formed after laser ablation through collisions with an inert bath gas that allow the ions to be landed at energies below 1 eV onto substrates. The split-ring ion optic is capable of directing ions toward the detector or a landing substrate for selected components.

Provided is an ion beam processing apparatus including an ion generation chamber, a processing chamber, and electrodes to form an ion beam by extracting ions generated in the ion generation chamber to the processing chamber. The electrodes includes a first electrode disposed close to the ion generation chamber and provided with an ion passage hole to allow passage of the ions, and a second electrode disposed adjacent to the first electrode and closer to the processing chamber than the first electrode is, and provided with an ion passage hole to allow passage of the ions. The apparatus also includes a power unit which applies different electric potentials to the first electrode and the second electrode, respectively, so as to accelerate the ions generated by an ion generator in the ion generation chamber. A material of the first electrode is different from a material of the second electrode.

A single beam plasma or ion source apparatus, including multiple and different power sources, is provided. An aspect of the present apparatus and method employs simultaneous excitation of an ion source by DC and AC, or DC and RF power supplies. Another aspect employs an ion source including multiple magnets and magnetic shunts arranged in a generally E cross-sectional shape.

An apparatus and method for the creation of negative ion beams is disclosed. The apparatus includes an RF ion source, having an extraction aperture. An antenna disposed proximate a dielectric window is energized by a pulsed RF power supply. While the RF power supply is actuated, a plasma containing primarily positive ions and electrons is created. When the RF power supply is deactivated, the plasma transforms into an ion-ion plasma. Negative ions may be extracted from the RF ion source while the RF power supply is deactivated. These negative ions, in the form of a negative ribbon ion beam, may be directed toward a workpiece at a specific incident angle. Further, both a positive ion beam and a negative ion beam may be extracted from the same ion source by pulsing the bias power supply multiple times each period.

An apparatus to generate negative hydrogen ions. The apparatus may include an ion source chamber having a gas inlet to receive H.sub.2 gas; a light source directing radiation into the ion source chamber to generate excited H.sub.2 molecules having an excited vibrational state from at least some of the H.sub.2 gas; a low energy electron source directing low energy electrons into the ion source chamber, wherein H.sup. ions are generated from at least some of the excited H.sub.2 molecules; and an extraction assembly arranged to extract the H.sup. ions from the ion source chamber.

An apparatus and method for the creation of negative ion beams is disclosed. The apparatus includes an RF ion source, having an extraction aperture. An antenna disposed proximate a dielectric window is energized by a pulsed RF power supply. While the RF power supply is actuated, a plasma containing primarily positive ions and electrons is created. When the RF power supply is deactivated, the plasma transforms into an ion-ion plasma. Negative ions may be extracted from the RF ion source while the RF power supply is deactivated. These negative ions, in the form of a negative ribbon ion beam, may be directed toward a workpiece at a specific incident angle. Further, both a positive ion beam and a negative ion beam may be extracted from the same ion source by pulsing the bias power supply multiple times each period.

The invention comprises a charged particle cancer therapy system used to seal a periphery of a tumor, such as through use of a proton or carbon ion beam searing the outer edges of the tumor, which prevents/hinders nutrient delivery to the tumor resultant in stunted growth of the tumor, halted growth of the tumor, and/or starvation/necrosis of the tumor. Optionally, a tumor sealing layer is formed using multiple passes, of a treatment beam of the charged particle cancer therapy system, across a tumor/healthy tissue boundary layer or voxel.

The present invention provides an inductively coupled, magnetically enhanced ion beam source, suitable to be used in conjunction with probe-forming optics to produce an ion beam without kinetic energy oscillations induced by the source.

An apparatus, referred to as a light bath, is disposed in a beamline ion implantation system and is used to photoionize particles in the ion beam into positively charged particles. Once positively charged, these particles can be manipulated by the various components in the beamline ion implantation system. In certain embodiments, a positively biased electrode is disposed downstream from the light bath to repel the formerly non-positively charged particles away from the workpiece. In certain embodiments, the light bath is disposed within an existing component in the beamline ion implantation system, such as a deceleration stage or a Vertical Electrostatic Energy Filter. The light source emits light at a wavelength sufficiently short so as to ionize the non-positively charged particles. In certain embodiments, the wavelength is less than 250 nm.