The present invention is related to an apparatus for transporting a charged particle beam. The apparatus may include means for scanning the charged particle beam on a target, a dipole magnet arranged upstream of the means for scanning, at least three quadrupole lenses arranged between the dipole magnet and the means for scanning and means for adjusting the field strength of said at least three quadrupole lenses in function of the scanning angle of the charged particle beam. The apparatus can be made at least single achromatic.

Disclosed herein is a composite charged particle beam apparatus including a focused ion beam column and an electron beam column, the apparatus preventing the electron beam column from being contaminated so as to emit an electron beam with high precision. The apparatus includes: a sample tray on which a sample is placed; a focused ion beam column irradiating the sample by using a focused ion beam; an electron beam column irradiating the sample by using an electron beam; a sample chamber receiving the sample tray, and the columns therein; an anti-contamination plate moving between an inserted position inserted into a space between a beam emission surface of the electron beam column and the sample tray, and an open position withdrawn from the space between the beam emission surface and the sample tray; and an operation unit operating the anti-contamination plate to move between the positions.

The objective of the present invention is to provide an ion beam device capable of forming a nanopyramid stably having one atom at the front end of an emitter tip even when the cooling temperature is lowered in order to observe a sample with a high signal-to-noise ratio. In the present invention, the ion beam device, wherein an ion beam generated from an electric field-ionized gas ion source is irradiated onto the sample to observe or process the sample, holds the temperature of the emitter tip at a second temperature higher than a first temperature for generating the ion beam and lower than room temperature, sets the extraction voltage to a second voltage higher than the first voltage used when generating the ion beam, and causes field evaporation of atoms at the front end of the emitter tip, when forming the nanopyramid having one atom at the front end of the emitter tip.

Apparatuses and methods directed toward endpoint detection are disclosed herein. An example method at least includes forming a plurality of lines on a top surface of a sample; removing, a plurality of times, material from a working surface of the sample, the working surface different than the top surface; imaging, a plurality of times, the sample to at least capture the plurality of lines; and determining an endpoint based on a relative spatial characteristic between two or more lines of the plurality of lines.

Methods for using a dual beam microscope system to simultaneously process a sample and image the processed portions of the sample, according to the present disclosure include the initial steps of emitting a plurality of electrons toward the sample, splitting the plurality of electrons into two electron beams, and then modifying the focal properties of at least one of the electron beams such that the two electron beams have different focal planes. Once the two beams have different focal planes, the first electron beam is focused such that it acts as a STEM beam. The STEM beam is then used to process a region of the sample to induce a physical change (e.g., perform milling, deposition, charge adjustment, phase change, etc.). The second electron beam is focused to act as a TEM beam to perform imaging of the region of the sample being processed

A writing data generating method for generating writing data used in a multi charged particle beam writing apparatus, that can suppress a data amount and a calculation amount in a multi charged particle beam writing apparatus generated from design data including a figure having a curve. The method includes calculating a pair of curves each representing a curve portion of a figure included in design data, the curves each being defined by a plurality of control points, and generating the writing data by expressing a position of a second control point adjacent in a traveling direction of the curve to a first control point of the plurality of control points as a displacement from the first control point in the traveling direction of the curve and a displacement from the first control point in a direction orthogonal to the traveling direction.

A method of evaluating a region of a sample that includes a first sub-region and a second sub-region, adjacent to the first sub-region, the region comprising a plurality of sets of vertically-stacked double-layers extending through both the first and second sub-regions with a geometry or orientation of the vertically-stacked double layers in the first sub-region being different than a geometry or orientation of the vertically-stacked double layers in the second region resulting in the first sub-region having a first milling rate and the second sub-region having a second milling rate different than the first milling rate, the method including: milling the region of a sample by scanning a focused ion beam over the region a plurality of iterations in which, for each iteration, the focused ion beam is scanned over the first sub-region and the second sub-region generating secondary electrons and secondary ions from each of the first and second sub-regions; detecting, during the milling, at least one of the generated secondary electrons or the secondary ions; generating, in real-time, an endpoint detection signal from the at least one of detected secondary electrons or secondary ions, the endpoint detection signal including a fast oscillating signal having a first frequency and a slow oscillating signal having a second frequency, slower than the first frequency; analyzing the fast and slow oscillating signals to determine original first and second frequencies of the fast and slow oscillating signals; and estimating, in real-time, a depth of each of the first and second sub-regions based on the determined first and second frequencies.

Reciprocal space map of specific sample locations is generated based on the sample images acquired by irradiating the sample with a charged particle beam at multiple incident angles. The incident angles are obtained by tilting the charged particle beam and/or the sample around two perpendicular axes within the sample plane. The reciprocal space map of a selected sample location is generated based on intensity of pixels corresponding to the location in the sample images.

Methods and systems for creating TEM lamella using image restoration algorithms for low keV FIB images are disclosed. An example method includes irradiating a sample with an ion beam at low keV settings, generating a low keV ion beam image of the sample based on emissions resultant from irradiation by the ion beam, and then applying an image restoration model to the low keV ion beam image of the sample to generate a restored image. The sample is then localized within the restored image, and a low keV milling of the sample is performed with the ion beam based on the localized sample within the restored image.

Apparatuses and methods directed toward endpoint detection are disclosed herein. An example method at least includes forming a plurality of lines on a top surface of a sample; removing, a plurality of times, material from a working surface of the sample, the working surface different than the top surface; imaging, a plurality of times, the sample to at least capture the plurality of lines; and determining an endpoint based on a relative spatial characteristic between two or more lines of the plurality of lines.