An observation apparatus and method that avoids drawbacks of a Lorentz method and observes a weak scatterer or a phase object with in-focus, high resolution, and no azimuth dependency, by a Foucault method observation using a hollow-cone illumination that orbits and illuminates an incident electron beam having a predetermined inclination angle, an electron wave is converged at a position (height) of an aperture plate downstream of a sample, and a bright field condition in which a direct transmitted electron wave of the sample passes through the aperture plate, a dark field condition in which the transmitted electron wave is shielded, and a Schlieren condition in which approximately half of the transmitted wave is shielded as a boundary condition of both of the above conditions are controlled, and a spatial resolution of the observation image is controlled by selecting multiple diameters and shapes of the opening of the aperture plate.

An electron microscope includes an electron source for emitting an electron beam, an illumination lens for focusing the beam, an aberration corrector for correcting aberrations, an illumination deflector assembly disposed between the illumination lens and the aberration corrector and operating to deflect the beam and to vary its tilt relative to a sample, a scanning deflector for scanning the sample with the beam, an objective lens, a detector for detecting electrons transmitted through the sample and producing an image signal, a control section for controlling the illumination deflector assembly, and an image generating section for receiving the image signal and generating a differential phase contrast (DPC) image. The tilt of the beam is varied by the illumination deflector assembly such that the image generating section generates a plurality of DPC images at different tilt angles of the beam and creates a final image based on the DPC images.

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 ϑ 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 ϑ 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 ϑ 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 θ relative to a surface normal of the substrates and form gratings in the grating material.

A system and method that is capable of measuring the incident angle of an ion beam, especially an ion beam comprising heavier ions, is disclosed. In one embodiment, X-rays, rather than ions, are used to determine the channeling direction. In another embodiment, the workpiece is constructed, at least in part, of a material having a high molecular weight such that heaver ion beams can be measured. Further, in another embodiment, the parameters of the ion beam are measured across an entirety of the beam, allowing components of the ion implantation system to be further tuned to create a more uniform beam.

An electron beam apparatus including: an electron beam source configured to generate an electron beam; a beam conversion unit including an aperture array configured to generate a plurality of beamlets from the electron beam, and a deflector unit configured to deflect one or more groups of the plurality of beamlets; and a projection system configured to project the plurality of beamlets onto an object, wherein the deflector unit is configured to deflect the one or more groups of the plurality of beamlets to impinge on the object at different angles of incidence, each beamlet in a group having substantially the same angle of incidence on the object.

An observation apparatus and method that avoids drawbacks of a Lorentz method and observes a weak scatterer or a phase object with in-focus, high resolution, and no azimuth dependency, by a Foucault method observation using a hollow-cone illumination that orbits and illuminates an incident electron beam having a predetermined inclination angle, an electron wave is converged at a position (height) of an aperture plate downstream of a sample and a bright field condition in which a direct transmitted electron wave of the sample passes through the aperture plate, a dark field condition in which the transmitted electron wave is shielded and a Schlieren condition in which approximately half of the transmitted wave is shielded as a boundary condition of both of the above conditions are controlled, and a spatial resolution of the observation image is controlled by selecting multiple diameters and shapes of the opening of the aperture plate.

A system and method that is capable of measuring the incident angle of an ion beam, especially an ion beam comprising heavier ions, is disclosed. In one embodiment, X-rays, rather than ions, are used to determine the channeling direction. In another embodiment, the workpiece is constructed, at least in part, of a material having a high molecular weight such that heaver ion beams can be measured. Further, in another embodiment, the parameters of the ion beam are measured across an entirety of the beam, allowing components of the ion implantation system to be further tuned to create a more uniform beam.