A method of forming a semiconductor device may include providing a semiconductor device structure. The semiconductor device structure may include semiconductor fins pitched at a fin pitch on a substrate and a mask, disposed over the semiconductor fins, the mask defining a plurality of openings. The semiconductor device structure may further include an isolation oxide disposed on the substrate, between the semiconductor fins. The method may further include directing angled ions into the at least one of the plurality of openings. The angled ions may form at least one trench between at least one pair of the semiconductor fins, in the substrate below the isolation oxide between the at least one pair of the semiconductor fins. Furthermore, a width within the substrate of the at least one trench is greater than a minimum fin pitch and greater than a width of the at least one trench above the substrate.

A semiconductor device and method is disclosed. In one example, the method for forming a semiconductor device includes forming a trench extending from a front side surface of a semiconductor substrate into the semiconductor substrate. The method includes forming of material to be structured inside the trench. Material to be structured is irradiated with a tilted reactive ion beam at a non-orthogonal angle with respect to the front side surface such that an undesired portion of the material to be structured is removed due to the irradiation with the tilted reactive ion beam while an irradiation of another portion of the material to be structured is masked by an edge of the trench.

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.

There is provided a technique that includes: imaging a gas supply hole configured to supply a plasma-converted gas into a process chamber by using an imaging device disposed in the process chamber; detecting a plasma emission intensity based on an image of the imaged gas supply hole; and determining at least one of whether abnormal plasma discharge has occurred and whether plasma flickering has occurred based on the detected plasma emission intensity.

Apparatus and methods are disclosed for employing an accelerated neutral beam derived from an accelerated gas cluster ion beam as a physical etching beam for providing reduced material mixing at the etched surface, compared to previous techniques. This results in the ability to achieve improved depth profile resolution in measurements by analytical instruments such as SIMS and XPS (or ESCA) analytical instruments.

A method may include providing a substrate, comprising a patterning layer. The method may include forming a first pattern of first linear structures in the patterning layer, the first linear structures being elongated along a first direction. The method may include forming a mask over the patterning layer, the mask comprising a second pattern of second linear structures, elongated along a second direction, forming a non-zero angle with respect to the first direction. The method may include selectively removing a portion of the patterning layer while the mask is in place, wherein a first etch pattern is formed in the patterning stack, the first etch pattern comprising a two-dimensional array of cavities. The method may include directionally etching the first etch pattern using an angled ion beam, wherein a second etch pattern is formed, comprising the two-dimensional array of cavities, elongated along the first direction.

A microscopy system for imaging a sample can include a scanning electron microscope system configured for imaging a surface layer of the sample and a focused ion beam system configured for generating an ion beam for milling the surface layer away from a sample after it has been imaged. A movable mechanical shutter can be configured to be moved automatically into a position between the sample and the scanning electron microscope system, so that when the electron beam is not imaging the sample the movable mechanical shutter is positioned between the sample and the scanning electron microscope system.

Provided herein are approaches for angle control of neutral reactive species ion beams. In one approach, a workpiece processing apparatus may include a plasma source operable to generate a plasma within a plasma chamber enclosed by a chamber housing, and an extraction plate coupled to the chamber housing. The extraction plate may include a plurality of channels for delivering one or more radical beams to a workpiece, wherein each of the plurality of channels has a lengthwise axis oriented at a non-zero angle relative to a perpendicular extending from a main surface of the workpiece, wherein each channel of the plurality of channels has a channel length and a channel width, and wherein the channel width varies along the channel length.

A method of extracting and accelerating ions is provided. The method includes providing a ion source. The ion source includes a chamber. The ion source further includes a first hollow cathode having a first hollow cathode cavity and a first plasma exit orifice and a second hollow cathode having a second hollow cathode cavity and a second plasma exit orifice, the first and second hollow cathodes being disposed adjacently in the chamber. The ion source further includes a first ion accelerator between and in communication with the first plasma exit orifice and the chamber. The first ion accelerator forms a first ion acceleration cavity. The ion source further includes a second ion accelerator between and in communication with the second plasma orifice and the chamber. The second ion accelerator forms a second ion acceleration cavity. The method further includes generating a plasma using the first hollow cathode and the second hollow cathode. The first hollow cathode and the second hollow cathode are configured to alternatively function as electrode and counter-electrode. The method further includes extracting and accelerating ions. Each of the first ion acceleration cavity and the second ion acceleration cavity are sufficient to enable the extraction and acceleration of ions.

This invention relates to a method and a device for processing a surface of a substrate by means of a particle beam. The method comprises the irradiation of the surface of the substrate, wherein, in a first area of the surface of the substrate, the surface of the substrate is processed with the particle beam, which strikes the surface of the substrate in an unpulsed manner; and wherein, in a second area of the surface of the substrate, the surface of the substrate is processed with the particle beam, which strikes the surface of the substrate in a pulsed manner.