Analyzing a buried layer on a sample includes milling a spot on the sample using a charged particle beam of a focused ion beam (FIB) column to expose the buried layer along a sidewall of the spot. From a first perspective a first distance is measured between a first point on the sidewall corresponding to an upper surface of the buried layer and a second point on the sidewall corresponding to a lower surface of the buried layer. From a second perspective a second distance is measured between the first point on the sidewall corresponding to the upper surface of the buried layer and the second point on the sidewall corresponding to the lower surface of the buried layer. A thickness of the buried layer is determined using the first distance and the second distance.

In order to allow detecting backscattered electrons (BSEs) generated from the bottom of a hole for determining whether a hole with a super high aspect ratio is opened or for inspecting and measuring the ratio of the top diameter to the bottom diameter of a hole, which are typified in 3D-NAND processes of opening a hole, a primary electron beam accelerated at a high accelerating voltage is applied to a sample. Backscattered electrons (BSEs) at a low angle (e.g. a zenith angle of five degrees or more) are detected. Thus, the bottom of a hole is observed using “penetrating BSEs” having been emitted from the bottom of the hole and penetrated the side wall. Using the characteristics in which a penetrating distance is relatively prolonged through a deep hole and the amount of penetrating BSEs is decreased to cause a dark image, a calibration curve expressing the relationship between a hole depth and the brightness is given to measure the hole depth.

An object of the present invention is to provide a charged particle beam device which can realize improved contrast of an elongated pattern in a specific direction, such as a groove-like pattern. In order to achieve the above-described object, the present invention proposes a charged particle beam device including a detector for detecting a charged particle obtained based on a charged particle beam discharged to a sample. The charged particle beam device includes a charged particle passage restricting member that has at least one of an arcuate groove and a groove having a longitudinal direction in a plurality of directions, and a deflector that deflects the charged particle discharged toward the groove from the sample. The charged particle discharged from the sample is deflected to a designated position of the groove.

The present disclosure pertains to a method, a system, and a computer-readable medium for highly precisely measuring the depth of a recess formed in a sample even when, inter alia, the material or pattern density of the sample differs. In order to achieve the purpose described above, there are proposed a method, a measurement system, and a non-temporary computer-readable medium for storing program commands that can be executed by a computer system, the method, system, and medium involving: using a measurement tool to acquire an image or a brightness distribution of a region including a recess formed in a sample; extracting a first characteristic of the interior of the recess, and a second characteristic pertaining to the dimensions or area of the recess, from the acquired image or brightness distribution; and inputting the extracted first characteristic and second characteristic to a model that indicates the relationship between the first characteristic, the second characteristic, and a depth index of the recess to thereby derive the depth index of the recess.

The present invention has a computation device for measuring the dimensions of patterns formed on a sample on the basis of a signal obtained from a charged particle beam device. The computation device has a positional deviation amount calculation unit for calculating the amount of positional deviation in a direction parallel to a wafer surface between two patterns having different heights on the basis of an image acquired at a given beam tilt angle; a pattern inclination amount calculation unit for calculating an amount of pattern inclination from the amount of positional deviation using a predetermined relational expression for the amount of positional deviation and the amount of pattern inclination; and a beam tilt control amount calculation unit for controlling the beam tilt angle so as to match the amount of pattern inclination. The pattern measurement device sets the beam tilt angle to a calculated beam tilt angle, reacquires an image and measures the patterns.

In the present invention, an electro-optical condition generation unit includes: a condition setting unit that sets, as a plurality of electro-optical conditions, a plurality of electro-optical conditions in which the combinations of the aperture angle and the focal-point height for an electron beam are different; an index calculating unit that determines a measurement-performance index in the electro-optical conditions set by the condition setting unit; and a condition deriving unit that derives an electro-optical condition, including an aperture angle and a focal-point height, so that the measurement-performance index determined by the index calculating unit becomes a prescribed value.

A UI image includes a reference image, which includes a background image and a schematic image. The background image corresponds to a cross section of a specimen having a multilayer structure. The schematic image includes a figure indicating an electron penetration depth, a figure indicating a characteristic X-ray generation depth, and a figure indicating a back-scattered electron generation depth. These figures are displayed in an overlapping manner or in parallel to each other.

A scanning electron microscope apparatus including an electron gun configured to generate an electron beam, a focusing lens configured to concentrate the electron beam from the electron gun, an electron detector configured to detect signals emitted from a sample in response to the electron beam incident on the sample, a stage configured to receive the sample thereon, and a focus calibration structure on an upper part of the stage.

A fast method of imaging a 2D sample with a multi-beam particle microscope includes the following steps: providing a layer of the 2D sample; determining a feature size of features included in the layer; determining a pixel size based on the determined feature size in the layer; determining a beam pitch size between individual beams in the layer based on the determined pixel size; and imaging the layer of the 2D sample with a setting of the multi-beam particle microscope based on the determined pixel size and based on the determined beam pitch size.

A charged particle beam apparatus for inspecting a sample is provided. The apparatus includes a pixelized electron detector to receive signal electrons generated in response to an incidence of an emitted charged particle beam onto the sample. The pixelized electron detector includes multiple pixels arranged in a grid pattern. The multiple pixels may be configured to generate multiple detection signals, wherein each detection signal corresponds to the signal electrons received by a corresponding pixel of the pixelized electron detector. The apparatus further includes a controller includes circuitry configured to determine a topographical characteristic of a structure within the sample based on the detection signals generated by the multiple pixels, and identifying a defect within the sample based on the topographical characteristic of the structure of the sample.