Provided herein are deposition systems utilizing coated grids in an ion deposition process which provide more predictable erosion of the coating rather than erosion of the grid itself. Further, coatings may be utilized in which the coating material does not act as a contaminant to the deposition process, thereby eliminating contamination of the sample surface due to deposition of unwanted grid material. Also provided are methods of refurbishing a coated grid by periodically replacing the coating material thus protecting the grid itself and allowing a grid to be used indefinitely.

Lithographic apparatuses suitable for complementary e-beam lithography (CEBL) are described. In an example, a method of forming a pattern for a semiconductor structure includes forming a pattern of parallel lines above a substrate. The method also includes aligning the substrate in an e-beam tool to provide the pattern of parallel lines parallel with a scan direction of the e-beam tool. The e-beam tool includes a column having a blanker aperture array (BAA) with a staggered pair of columns of openings along an array direction orthogonal to the scan direction. The method also includes forming a pattern of cuts or vias in or above the pattern of parallel lines to provide line breaks for the pattern of parallel lines by scanning the substrate along the scan direction. A cumulative current through the column has a non-zero and substantially uniform cumulative current value throughout the scanning.

An apparatus for processing a specimen with two or more particle beams, wherein the specimen has a milled side that is processed by a first particle beam and observed by a second particle beam. The specimen is milled during a first milling operation by the first particle beam with the specimen in a first position. Thereafter, the specimen tilts in a second position around an axis of tilt of the specimen. Thereafter, the specimen is milled during a second milling operation. Milling can be performed during continuous tilting of the specimen around the axis of tilt. The axis of tilt of the specimen intersects the milled side. In all the aforementioned positions of the specimen, the second particle beam impinges on the milled side, which enables monitoring of the milling in real time.

Embodiments herein are directed to a resonator for an ion implanter. In some embodiments, a resonator may include a housing, and a first coil and a second coil partially disposed within the housing. Each of the first and second coils may include a first end including an opening for receiving an ion beam, and a central section extending helically about a central axis, wherein the central axis is parallel to a beamline of the ion beam, and wherein an inner side of the central section has a flattened surface.

A method for detecting a discharge site for a charged particle beam emitting apparatus includes switchable first and second modes. The first mode enables a beam of charged particles to be deflected by applying voltages to electrodes. The second mode enables acquisition of data items indicative of potential of each of the electrodes while the beam is being emitted without applying the voltages. The method includes, in the second mode, detecting an occurrence of a discharge when a fluctuation in potential indicated by data items relating to one of the electrodes exceeds a predetermined threshold value; and detecting a site corresponding to the electrode, as a site having an occurrence of the discharge.

An aperture diaphragm capable of varying the size of an aperture in two dimensions is disclosed. The aperture diaphragm may be utilized in an ion implantation system, such as between the mass analyzer and the acceleration column. In this way, the aperture diaphragm may be used to control at least one parameter of the ion beam. These parameters may include angular spread in the height direction, angular spread in the width direction, beam current or cross-sectional area. Various embodiments of the aperture diaphragm are shown. In certain embodiments, the size of the aperture in the height and width directions may be independently controlled, while in other embodiments, the ratio between height and width is constant.

The disclosure relates to an electron-optical module of an electron-optical apparatus. The electron-optical module comprises a vacuum chamber, a high voltage shielding arrangement located within the vacuum chamber, and an aperture array configured to form a plurality of beamlets from an electron beam and located within the high voltage shielding arrangement. Wherein the electron-optical module can be configured to be removable from the electron-optical apparatus.

Provided is a sample loading method of loading a cooled sample into a sample exchange chamber of a charged particle beam apparatus includes: attaching the sample container in which a sample and liquid nitrogen are accommodated to the sample exchange chamber via a gate valve; evacuating a space between a liquid surface of the liquid nitrogen and the gate valve in a state in which the gate valve is closed; discharging the liquid nitrogen in the sample container after the space between the liquid surface of the liquid nitrogen and the gate valve has been evacuated; evacuating a space in the sample container after the liquid nitrogen in the sample container has been discharged; and opening the gate valve after the space in the sample container has been evacuated.

A charged particle buncher includes a series of spaced apart electrodes arranged to generate a shaped electric field. The series includes a first electrode, a last electrode and one or more intermediate electrodes. The charged particle buncher includes a waveform device attached to the electrodes and configured to apply a periodic potential waveform to each electrode independently in a manner so as to form a quasi-electrostatic time varying potential gradient between adjacent electrodes and to cause spatial distribution of charged particles that form a plurality of nodes and antinodes. The nodes have a charged particle density and the antinodes have substantially no charged particle density, and the nodes and the antinodes are formed from a charged particle beam configured to hit the target.

A method of milling a sample that includes a first layer formed over a second layer, where the first and second layers are different materials, the method comprising: milling the region of the sample by scanning a focused ion beam over the region a plurality of iterations in which, for each iteration, the focused ion beam removes material from the sample generating byproducts from the milled region; detecting, during the milling, the partial pressures of one or more byproducts with a residual gas analyzer positioned to have a direct line of sight to the milled region; generating, in real-time, an output detection signal from the residual gas analyzer indicative of an amount of the one or more byproducts detected; and stopping the milling based on the output signal.