A charged particle beam source for a surface processing apparatus is disclosed. The charged particle beam source comprises: a plasma chamber; a plasma generation unit adapted to convert an input gas within the plasma chamber into a plasma containing charged particles; and a grid assembly adjacent an opening of the plasma chamber. The grid assembly comprises one or more grids each having a plurality of apertures therethrough, the one or more grids being electrically biased in use so as to accelerate charged particles from the plasma through the grid(s) to thereby output a charged particle beam, the major axis of which is substantially perpendicular to the plane of the grid assembly. The transmissivity of the or each grid to the charged particles is defined by the relative proportion of aperture area to non-aperture area, and at least one of the grids has a transmissivity which varies across the grid along a first direction, the transmissivity being lower adjacent a first extremity of the grid than adjacent a second extremity of the grid opposite the first extremity, the first direction lying parallel to the plane of the grid assembly, such that in use the charged particle beam output by the source has a non-uniform charged particle current density profile in a plane parallel to the plane of the grid assembly which varies along the first direction, the charged particle current density being lower adjacent a first edge of the beam than adjacent a second edge of the beam opposite the first edge.

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.

Apparatus for a multi-source ion beam etching (IBE) system are provided herein. In some embodiments, a multi-source IBE system includes a multi-source lid comprising a multi-source adaptor and a lower chamber adaptor, a plurality of IBE sources coupled to the multi-source adaptor, a rotary shield assembly coupled to a shield motor mechanism configured to rotate the rotary shield, wherein the shield motor mechanism is coupled to a top portion of the multi-source lid, and wherein the rotary shield includes a body that has one IBE source opening formed through the body, and at least one beam conduit that engages the one IBE source opening in the rotary shield on one end, and engages the bottom portion of the IBE sources on the opposite end of the beam conduit.

Systems for and methods for generating precise structure reconstruction using slice and view images, are disclosed. An example method comprises, obtaining a slice and view images of a sample that depicts a 3D fiducial and cross-sections of a structure in the sample. The 3D fiducial is configured such that when a layer of material having a uniform thickness is removed from a surface of the sample that includes the 3D fiducial the cross-sectional shape of the 3D fiducial in the new surface is consistent. Relative positions are determined between the 3D fiducial the cross-sections of the structure in individual images. Positional relationships are then determined between the cross-sections of the structure in different images in a common reference frame based on the relative positions.

According to the present invention, writing data capable of suppressing a data amount and a calculation amount in a multi charged particle beam writing apparatus is generated from design data including a figure having a curve. The present embodiment relates to a writing data generating method for generating writing data used in a multi charged particle beam writing apparatus. The method includes calculating a pair of curves each representing a curve portion of a figure included in design data, the curves each being defined by a plurality of control points, and generating the writing data by expressing a position of a second control point adjacent in a traveling direction of the curve to a first control point of the plurality of control points as a displacement from the first control point in the traveling direction of the curve and a displacement from the first control point in a direction orthogonal to the traveling direction.

An improved ANAB system or process substantially or fully eliminating contaminant particles from reaching a beam target by adding to the usual primary (first) ionizer of the ANAB system or process an additional (second) ionizer to ionize contaminant particles and means to block or retard the ionized particles to prevent their reaching the beam target.

One or more layers of a magnetic random access memory (MRAM) stack on a substrate are etched by ion beam etching. An ion beam of an inert gas is generated in an ion beam source chamber and applied to a substrate in a continuous or pulsed manner. Without passing through the ion beam source chamber, a reactive gas is flowed directly into a processing chamber in which the substrate is located, where the reactive gas is pulsed or continuously provided into the processing chamber. The reactive gas may include a carbon-containing gas having a hydroxyl group that is flowed towards the substrate to limit re-deposition of sputtered atoms on exposed surfaces of the substrate from ion beam etching.

A miller, a non-transitory computer readable medium, and a method. The miller may include an ion beam column that may be configured to form a vertical surface in an object by applying a milling process that may include forming a vertical surface by irradiating, for a certain period of time, an area of an upper surface of an object by a defocused ion beam that comprises multiple rays. During the certain period of time and at a plane of the upper surface of the object, a majority of the multiple rays are closer to an edge of the defocused ion beam than to a center of the defocused ion beam. The focal plane of the defocused ion beam is located below the upper surface of the object.

Redeposition of substrate material on a fiducial resulting from charged particle beam (CPB) or laser beam milling of a substrate can be reduced with a shield formed on the substrate surface. The shield typically has a suitable height that can be selected based on proximity of an area to be milled to the fiducial. The shield can be formed with the milling beam using beam-assisted chemical vapor deposition (CVD). The same or different beams can be used for milling and beam-assisted CVD.

Embodiments described herein relate to methods of forming gratings with different slant angles on a substrate and forming gratings with different slant angles on successive substrates using angled etch systems. The methods include positioning portions of substrates retained on a platen in a path of an ion beam. The substrates have a grating material disposed thereon. The ion beam is configured to contact the grating material at an ion beam angle θ relative to a surface normal of the substrates and form gratings in the grating material. The substrates are rotated about an axis of the platen resulting in rotation angles ϕ between the ion beam and a surface normal of the gratings. The gratings have slant angles θ′ relative to the surface normal of the substrates. The rotation angles ϕ selected by an equation ϕ=cos.sup.−1(tan(θ′)/tan(θ)).