The present invention discloses an ion beam lithography method based on an ion beam lithography system. The ion beam lithography system includes a roll-roll printer placed in a vacuum, and a medium-high-energy wide-range ion source, a medium-low-energy wide-range ion source and a low-energy ion source installed on the roll-roll printer. The ion beam lithography method includes: first coating a polyimide (PI) substrate with a dry film, etching the dry film according to a preset circuit pattern, then using the ion beam lithography system to deposit a wide-energy-range metal ion on the circuit pattern to form a film substrate, and finally stripping the dry film off the film substrate to obtain a printed circuit board (PCB).

The present disclosure relates to an ion beam etching (IBE) system including a process chamber. The process chamber includes a plasma chamber configured to provide plasma. In addition, the process chamber includes an accelerator grid having multiple accelerator grid elements including a first accelerator grid element and a second accelerator grid element. A first wire is coupled to the first accelerator grid element and configured to supply a first voltage to the first accelerator grid element. A second wire is coupled to the second accelerator grid element and configured to supply a second voltage to the second accelerator grid element, where the second voltage is different from the first voltage. A first ion beam through a first hole is controlled by the first accelerator grid element, and a second ion beam through a second hole is controlled by the second accelerator grid element.

An ion source capable of extracting a ribbon ion beam with improved uniformity is disclosed. One of the walls of the ion source has a protrusion on its interior surface facing the chamber. The protrusion creates a loss area that serves as a sink for free electrons and ions. This causes a reduction in plasma density near the protrusion, and may improve the uniformity of the ribbon ion beam that is extracted from the ion source by modifying the beam current near the protrusion. The shape of the protrusion may be modified to achieve the desired uniformity. The protrusion may also be utilized with a cylindrical ion source. In certain embodiments, the protrusion is created by a plurality of mechanically adjustable protrusion elements.

The present disclosure relates to systems and methods of additive manufacturing that reduce or eliminates defects in the bulk deposition material microstructure resulting from the additive manufacturing process. An additive manufacturing system comprises evaporating a deposition material to form an evaporated deposition material and ionizing the evaporated deposition material to form an ionized deposition material flux. After forming the ionized deposition material flux, the ionized deposition material flux is directed through an aperture, accelerated to a controlled kinetic energy level and deposited onto a surface of a substrate. The aperture mechanism may comprise a physical, electrical, or magnetic aperture mechanism. Evaporation of the deposition material may be performed with an evaporation mechanism comprised of resistive heating, inductive heating, thermal radiation, electron heating, and electrical arc source heating.

An ion source having an electrically isolated extraction plate is disclosed. By isolating the extraction plate, a different voltage can be applied to the extraction plate than to the body of the arc chamber. By applying a more positive voltage to the extraction plate, more efficient ion source operation with higher plasma density can be achieved. In this mode the plasma potential is increased, and the electrostatic sheath reduces losses of electrons to the chamber walls. By applying a more negative voltage, an ion rich sheath adjacent to the extraction aperture can be created. In this mode, conditioning and cleaning of the extraction plate is achieved via ion bombardment. Further, in certain embodiments, the voltage applied to the extraction plate can be pulsed to allow ion extraction and cleaning to occur simultaneously.

An ion source uses at least one induction coil to generate ac magnetic field to couple rf/VHF power into a plasma within a vessel, where the excitation coil may be a single set of turns each turn having lobes or multiple separate sets of windings. The excitation coil is positioned outside and proximate that side of the vessel that is opposite to the extraction slit, and elongated parallel to the length dimension of the extraction slit. The conducting shield(s) positioned outside or integrated with the well of the vessel are used to block the capacitive coupling to the plasma and/or to collect any rf/VHF current may be coupled into the plasma. The conducting shield positioned between the vessel and the coil set can either shield the plasma from capacitive coupling from the excitation coils, or be tuned to have a higher rf/VHF voltage to ignite or clean the source.

The presently disclosed ion sources include one or more electromagnets for changing the distribution of plasma within a discharge space of an ion source. At least one of the electromagnets is oriented about an outer periphery of a tubular sidewall of the ion source and changes a distribution of the plasma in a peripheral region of the discharge space.

A plasma ion source includes: a gas introduction chamber, into which raw gas is introduced; a plasma generation chamber connected to the gas introduction chamber and made of a dielectric material; a coil wound along an outer circumference of the plasma generation chamber and to which high-frequency power is applied; an envelope surrounding the gas introduction chamber, the plasma generation chamber and the coil; and insulating liquid filled inside the gas introduction chamber, the plasma generation chamber and the envelope to immerse the coil and having an dielectric strength voltage relatively greater than that of the envelope and the same dielectric dissipation factor as the plasma generation chamber.

A rotatable targeting magnet apparatus and method of use thereof is described where the rotatable targeting magnet rotates independently of a beamline arc at the end of the beamline arc, where the arc is after an accelerator and before the patient in a cancer therapy system. The rotatable targeting magnet directs the charged particle beam, such as vertically, using applied current to the targeting magnet while rotation of the magnet allows scanning across the tumor. Rotation of the patient relative to the charged particle allows distribution of trailing Bragg peak energy within and/or circumferentially about the tumor.

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.