Embodiments described herein relate to methods and apparatus for forming gratings having a plurality of fins with different slant angles on a substrate and forming fins with different slant angles on successive substrates using angled etch systems and/or an optical device. 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 relative to a surface normal of the substrates and form gratings in the grating material.

Embodiments described herein relate to methods and apparatus for forming gratings having a plurality of fins with different slant angles on a substrate and forming fins with different slant angles on successive substrates using angled etch systems and/or an optical device. 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 relative to a surface normal of the substrates and form gratings in the grating material.

A method of patterning a substrate. The method may include providing a cavity in a layer, disposed on the substrate, the cavity having a first length along a first direction and a first width along a second direction, perpendicular to the first direction, and wherein the layer has a first height along a third direction, perpendicular to the first direction and the second direction. The method may include depositing a sacrificial layer over the cavity in a first deposition procedure; and directing angled ions to the cavity in a first exposure, wherein the cavity is etched, and wherein after the first exposure, the cavity has a second length along the first direction, greater than the first length, and wherein the cavity has a second width along the second direction, no greater than the first width.

Systems and methods of imaging a sample using a tilted charged-particle beam. The apparatus may comprise a first deflector located between the charged-particle source and an objective lens and configured to deflect the charged-particle beam away from the primary optical axis; a second deflector located substantially at a focal plane of the objective lens and configured to deflect the charged-particle beam back towards the primary optical axis; and a third deflector located substantially at a principal plane of the objective lens, wherein the third deflector is configured to shift a wobbling center of the objective lens to an off-axis wobbling location, and wherein the first and the second deflectors are configured to deflect the charged-particle beam to pass through the off-axis wobbling location to land on a surface of a sample at a first landing location and having a beam-tilt angle.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit forms plural and parallel images of one single electron source by deflecting plural beamlets of a parallel primary-electron beam therefrom, and one objective lens focuses the plural deflected beamlets onto a sample surface and forms plural probe spots thereon. A movable condenser lens is used to collimate the primary-electron beam and vary the currents of the plural probe spots, a pre-beamlet-forming means weakens the Coulomb effect of the primary-electron beam, and the source-conversion unit minimizes the sizes of the plural probe spots by minimizing and compensating the off-axis aberrations of the objective lens and condenser lens.

A method for reducing throughput time in a sample image acquisition session in transmission electron microscopy comprises: providing an electron microscope comprising a sample component, a beam generator, an adjusting component, and a filtering component; securing a sample by using the sample component; generating an electron beam by using the beam generator; generating an image beam by directing the beam to the sample component; adjusting at least one of the beam and the image beam by using the adjusting component to obtain at least one modified image beam, wherein the adjusting is performed in such a way, that off-axial aberration of the modified image beam is minimized; and filtering the modified image beam via the filtering component to reduce resolution-deteriorating effect of chromatic aberration on the modified image beam resulting from the adjusting of the at least one of the beam and the image beam.

A charged particle beam device includes an electron source which generates an electron beam, an objective lens which is applied with a coil current to converge the electron beam on a sample, a control unit which controls the current to be applied to the objective lens, a hysteresis characteristic storage unit which stores hysteresis characteristic information of the objective lens, a history information storage unit which stores history information related to the coil current, and an estimation unit which estimates a magnetic field generated by the objective lens on the basis of the coil current, the history information, and the hysteresis characteristic information.

Techniques for high throughput electron channeling contrast imaging (ECCI) by varying electron beam energy are provided. In one aspect, a method for ECCI of a crystalline wafer includes: placing the crystalline wafer under an electron microscope having an angle of less than 90 relative to a surface of the crystalline wafer; generating an electron beam, by the electron microscope, incident on the crystalline wafer; varying an accelerating voltage of the electron microscope to access a channeling condition of the crystalline wafer; and obtaining an image of the crystalline wafer. A system for ECCI is also provided.

A method of characterizing a region in a sample under study, and related systems, is disclosed. In once aspect, the sample under study comprises a first region having first crystalline properties and a second region having second crystalline properties. The method comprises irradiating the sample under study with an electron beam, the average relative angle between the electron beam and the sample under study being selected so that a contribution in the backscattered or forward scattered signal of the first region is distinguishable from that of the second region. The method further comprises detecting the backscattered or forward scattered electrons, and deriving a characteristic of the first and/or the second region from the detected backscattered or forward scattered electrons. The instantaneous relative angle between the electron beam and the sample under study is modulated with a predetermined modulation frequency during the irradiating the sample under study with an electron beam. Detecting the backscattered or forward scattered electrons is performed at the predetermined modulation frequency.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit forms plural and parallel images of one single electron source by deflecting plural beamlets of a parallel primary-electron beam therefrom, and one objective lens focuses the plural deflected beamlets onto a sample surface and forms plural probe spots thereon. A movable condenser lens is used to collimate the primary-electron beam and vary the currents of the plural probe spots, a pre-beamlet-forming means weakens the Coulomb effect of the primary-electron beam, and the source-conversion unit minimizes the sizes of the plural probe spots by minimizing and compensating the off-axis aberrations of the objective lens and condenser lens.