Disclosed herein is a computer-based method for non-destructive depth-profiling of samples. The method includes a measurement operation and a data analysis operation. The measurement operation includes, for each of a plurality of landing energies: (i) projecting an electron beam on a sample, which penetrates the sample to a respective depth determined by the landing energy, and (ii) sensing electrons returned from the sample, thereby obtaining a respective sensed electrons data set. The data analysis operation includes generating from the sensed electrons data sets a concentration map, which characterizing at least a vertical dimension of the sample.

Multi-beam effects which reduce the accuracy, or the speed of a wafer inspection are corrected dependent on an inspection position using an improved multi-beam system and a wafer inspection method using the multi-beam system. The multi-beam system comprises a mechanism for influencing and homogenising an extraction field dependent on the inspection position, for example dependent on a distance from a wafer edge.

A particle-beam inspection system may include a reflective particle-beam imaging system providing an image of a selected portion of a sample and a diffraction pattern of the selected portion of the sample and a controller communicatively coupled to the reflective particle-beam imaging system. The controller may receive two or more sample-plane images from the reflective particle-beam imaging system associated with two or more selected portions of the sample, where at least some of the two or more selected portions of the sample overlap. The controller may further receive two or more diffraction-plane images from the reflective particle-beam imaging system associated with the two or more selected portions of the sample. The controller may further construct one or more output images of the two or more selected portions of the sample from the two or more diffraction-plane images using phase information obtained from the two or more sample-plane images.

A method for crystal analysis includes identifying a crystalline region on a device where an electronic channeling pattern is needed to be determined, acquiring a whole image for each of a plurality of different positions for the crystalline region using a scanning electron microscope (SEM) as the crystalline region is moved to different positions. Relevant regions are extracted from the whole images. The images of the relevant regions are stitched together to form a composite map of a full electron channeling pattern representative of the crystalline region wherein the electronic channeling pattern is provided due to an increase in effective angular range between a SEM beam and a surface of the crystal region.

Provided is a charged particle beam device that enables, even if a visual field includes therein a plurality of regions having different secondary electron emission conditions, the setting of appropriate energy filter conditions adapted to each of these regions. The charged particle beam device is equipped with a detector for detecting charged particles obtained on the basis of scanning, over a sample, a charged particle beam emitted from a charged particle source, and an energy filter for filtering by energy the charged particles emitted from the sample. Index values are determined for the plurality of regions contained within the scanning region of the charged particle beam, and, for each of a plurality of energy filter conditions, differences are calculated between the plurality of index values and the reference index values that have been set for each of the plurality of regions.

An electron reflectometer includes: a sample stage; a source that produces source electrons; a source collimator; and an electron detector that receives collimated reflected electrons.

A method for crystal analysis includes identifying a crystalline region on a device where an electronic channeling pattern is needed to be determined, acquiring a whole image for each of a plurality of different positions for the crystalline region using a scanning electron microscope (SEM) as the crystalline region is moved to different positions. Relevant regions are extracted from the whole images. The images of the relevant regions are stitched together to form a composite map of a full electron channeling pattern representative of the crystalline region wherein the electronic channeling pattern is provided due to an increase in effective angular range between a SEM beam and a surface of the crystal region.

An electron microscope system and a method of measuring an aberration of the electron microscope system are disclosed. A method of controlling an aberration of an electron microscope includes obtaining a dispersed energy distribution for electrons at a diffraction plane of the electron microscope and placing an aperture at a selected location of the dispersed energy distribution in the diffraction plane. The method measures displacement of an image of the aperture in an image plane of the electron microscope for the selected location of the aperture. The method determines an aberration coefficient of the electron microscope from the measured displacement and the selected location of the aperture and alters a parameter of an element of the electron microscope to control the aberration of the electron microscope based at least in part on the determined aberration coefficient.

Disclosed is a composite beam apparatus capable of suppressing the influence of charge build-up, or electric field or magnetic field leakage from an electron beam column when subjecting a sample to cross-section processing with a focused ion beam and then performing finishing processing with another beam. The Composite beam apparatus includes: an electron beam column irradiating an electron beam onto a sample; a focused ion beam column irradiating a focused ion beam onto the sample to form a cross section; a neutral particle beam column having an acceleration voltage set lower than that of the focused ion beam column, and irradiating a neutral particle beam onto the sample to perform finish processing of the cross section, wherein the electron beam column, the focused ion beam column, and the neutral particle beam column are arranged such that the beams of the columns cross each other at an irradiation point.

A secondary projection imaging system in a multi-beam apparatus is proposed, which makes the secondary electron detection with high collection efficiency and low cross-talk. The system employs one zoom lens, one projection lens and one anti-scanning deflection unit. The zoom lens and the projection lens respectively perform the zoom function and the anti-rotating function to remain the total imaging magnification and the total image rotation with respect to the landing energies and/or the currents of the plural primary beamlets. The anti-scanning deflection unit performs the anti-scanning function to eliminate the dynamic image displacement due to the deflection scanning of the plural primary beamlets.