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.

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.

In an electron beam apparatus performing angular scanning that changes an incident angle of an electron beam incident at a predetermined incident position on a sample, when a correction coil is provided in a gap portion of a yoke (magnetic path) of an objective lens, spherical aberration can be corrected by following a deflection signal even if a deflection frequency increases. Therefore, a main control unit that controls an electron optical system sets predetermined phase change amounts a, b with respect to control of a scanning coil in control of the correction coil, and the predetermined phase change amounts a, b are made different depending on a plurality of scanning modes having different scanning speeds.

A charged particle beam apparatus has a chamber configured to accommodate a sample with. An inside of the chamber is decompressed. A tube having an opening is disposed in the chamber, and introduces a mixed gas having a plurality of types of gases, in a direction towards the sample. A first beam generator emits a charged particle beam toward at least one of a region between an opening of the tube and the sample, or a region of the sample against which the mixed gas collides. A mixed gas generator provides the mixed gas to the tube. The opening of the tube has an elongated shape in a cross section in a direction substantially perpendicular to a flow direction of the mixed gas.

To implement a calibration sample by which an incident angle can be measured with high accuracy, an electron beam adjustment method, and an electron beam apparatus using the calibration sample. To adjust an electron beam using a calibration sample, the calibration sample includes a silicon single crystal substrate 201 whose upper surface is a {110} plane, a first recess structure 202 opening in the upper surface and extending in a first direction, and a second recess structure 203 opening in the upper surface and extending in a second direction intersecting the first direction, in which the first recess structure and the second recess structure each include a first side surface and a first bottom surface that intersects the first side surface, and a second side surface and a second bottom surface that intersects the second side surface, the first side surface and the second side surface are {111} planes, and the first bottom surface and the second bottom surface are crystal planes different from the {110} planes.

The present disclosure makes it possible to shorten the time required for measurement of a sample and to measure the sample with high throughput. A charged particle beam apparatus includes a storage device that stores a correction value table corresponding to a recipe and a computer system that executes measurement on a plurality of measurement points of a sample according to a measurement order determined in the recipe. The computer system stores, when executing the recipe on a first sample, an adjustment result of one or more imaging conditions in the correction value table at each of a plurality of measurement points of the first sample, and adjusts, when executing the recipe on a second sample different from the first sample, the imaging condition based on the adjustment result of the one or more imaging conditions stored in the correction value table at each of the plurality of measurement points.

A process for the preparation and imaging of a sample of rock from an oil and gas reservoir is provided. A sample of reservoir rock may be obtained, such as from a core sample obtained using a core sampling tool inserted in a wellbore extending into an oil and gas reservoir. A photoresist may be deposited on the surface of reservoir rock sample to form a homogenous layer. The photoresist-coated surface of the reservoir rock sample may be imaged using a focused ion beam (FIB). The photoresist protects the pores and other surface features of the rock from damage or implantation by the FIB ion beam and thus minimizes the curtain effect in the resulting images.

A charged particle beam apparatus has a chamber configured to accommodate a sample with. An inside of the chamber is decompressed. A tube having an opening is disposed in the chamber, and introduces a mixed gas having a plurality of types of gases, in a direction towards the sample. A first beam generator emits a charged particle beam toward at least one of a region between an opening of the tube and the sample, or a region of the sample against which the mixed gas collides. A mixed gas generator provides the mixed gas to the tube. The opening of the tube has an elongated shape in a cross section in a direction substantially perpendicular to a flow direction of the mixed gas.

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.

The disclosed technology relates to an apparatus for tomographic analysis of a specimen based on STEM images of the specimen, as well as for tomographic analysis of the chemical composition of the specimen based on X-ray detection by EDS detectors. In one aspect, the apparatus comprises an elongated specimen holder that is rotatable about a longitudinal axis and is configured to hold a pillar-shaped specimen at the end of the holder. The longitudinal axis is positioned in a sample plane which is perpendicular to the beam direction of an electron beam produced by an electron gun. The apparatus also comprises at least two EDS detectors, each EDS detector having a detecting surface oriented perpendicularly to the sample plane and intersecting with the sample plane, wherein the two EDS detectors are positioned on opposite lateral sides of the specimen.