Provided is a technique capable of achieving both throughput and robustness for a function of adjusting brightness (B) and contrast (C) of a captured image in a charged particle beam device. The charged particle beam device includes a computer system having a function (ABCC function) of adjusting the B and the C of an image obtained by imaging a sample. The computer system determines whether adjustment is necessary based on a result obtained by evaluating a first image obtained by imaging an imaging target of the sample (step S2), executes, when the adjustment is necessary based on a result of the determination, the adjustment on a second image of the imaging target to set an adjusted B value and an adjusted C value (step S4), and captures a third image of the imaging target based on the adjusted setting values to generate an image for observation (step S5).

A method of performing x-ray spectroscopy material analysis of a region of interest within a cross-section of a sample using an evaluation system that includes a focused ion beam (FIB) column, a scanning electron microscope (SEM) column, and an x-ray detector, including: forming a lamella having first and second opposing side surfaces in the sample by milling, with the FIB column, first and second trenches in the sample to expose the first and second sides surface of the lamella, respectively; depositing background material in the second trench, wherein the background material is selected such that the background material does not include any chemical elements that are expected to be within the region of interest of the sample; generating a charged particle beam with the SEM column and scanning the charged particle beam across a region of interest on the first side surface of the lamella such that the charged particle beam collides with the first side surface of the lamella at a non-vertical angle; and detecting x-rays generated while the region of interest is scanned by the charged particle beam.

The invention is to simplify operations performed when imaging an electron diffraction pattern by using a transmission electron microscope. As a solution to the problem, a transmission electron microscope includes a detector to which an electron diffraction pattern is projected, a mask for zero-order wave configured to be inserted into and pulled out from between a sample and the detector, and a current detector configured to be inserted into and pulled out from a detection region of the zero-order waves in a state where the mask is inserted. An amount of current of electron beams emitted to the mask is measured in real time, and the measurement result is automatically reflected in settings of imaging conditions of an imaging camera provided in the transmission electron microscope.

From a reference waveform 112 and a BSE signal waveform 211 that is extracted from a backscattered electron image and indicates a backscattered electron signal intensity from a pattern along a first direction, a difference waveform indicating a relationship between the backscattered electron signal intensity and a difference between a coordinate of the BSE signal waveform and a coordinate of the reference waveform which have the same backscattered electron signal intensity is generated, and presence or absence of a shielded region 203 that is not irradiated with a primary electron beam on a side wall of the pattern is determined based on the difference waveform. The reference waveform indicates a backscattered electron signal intensity from a reference pattern along the first direction in which the side wall is formed perpendicularly to an upper surface and a bottom surface of the pattern when the reference pattern is scanned with the primary electron beam.

A method to compensate for drift while controlling a charged particle beam (CPB) system having at least one charged particle beam controllable in position. Sources of drift include mechanical variations in the stage supporting the sample, beam deflection shifts, and environmental impacts, such as temperature. The method includes positioning a sample supported by a stage in the CPB system, monitoring a reference fiducial on a surface of the sample from a start time to an end time, determining a drift compensation to compensate for a drift that causes an unintended change in the position of a first charged particle beam relative to the sample by a known amount over a period of time based on a change in the position of the reference fiducial between the start time and the end time, and adjusting positions of the first charged particle beam by applying the determined drift compensation during an operation of the CPB system.

Embodiments may include methods, systems, and apparatuses for correcting a response function of an electron beam tool. The correcting may include modulating an electron beam parameter having a frequency; emitting an electron beam based on the electron beam parameter towards a specimen, thereby scattering electrons, wherein the electron beam is described by a source wave function having a source phase and a landing angle; detecting a portion of the scattered electrons at an electron detector, thereby yielding electron data including an electron wave function having an electron phase and an electron landing angle; determining, using a processor, a phase delay between the source phase and the electron phase, thereby yielding a latency; and correcting, using the processor, the response function of the electron beam tool using the latency and a difference between the source wave function and the electron wave function.

Roughness measurement corrects a machine difference utilizing first PSD data indicating power spectral density of a line pattern measured for a line pattern formed on a wafer for machine difference management by a reference machine in roughness index calculation and second PSD data indicating power spectral density of a line pattern measured for the line pattern formed on the wafer for machine difference management by a correction target machine are used to obtain a correction method for correcting the power spectral density of the second PSD data to the power spectral density of the first PSD data, power spectral density of a line pattern is measured as third PSD data from a scanning image of the line pattern, and corrected power spectral density obtained by correcting the power spectral density of the third PSD data by the obtained correction method is calculated.

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.

Provided is a charged particle beam apparatus that acquires an image by scanning a specimen with a charged particle beam, and includes a contrast adjustment circuit that adjusts contrast of the image; a brightness adjustment circuit that adjusts brightness of the image; and a control unit that controls the contrast adjustment circuit and the brightness adjustment circuit. The control unit acquires information on luminance of a reference image in a non-signal state, and information on an average value of luminance of each pixel of the reference image, controls the brightness adjustment circuit, based on the acquired information on luminance of the reference image in a non-signal state, acquires the image in a state where the brightness adjustment circuit is controlled, and adjusts the contrast of the acquired image by controlling the contrast adjustment circuit, based on the average value of luminance of each pixel of the reference image.

Methods include holding a sample with a movement stage configured to rotate the sample about a rotation axis, directing an imaging beam to a first sample location with the sample at a first rotational position about the rotation axis and detecting a first transmitted imaging beam image, rotating the sample using the movement stage about the rotation axis to a second rotational position, and directing the imaging beam to a second sample location by deflecting the imaging beam in relation to an optical axis of the imaging beam and detecting a second transmitted imaging beam image, wherein the second sample location is spaced apart from the first sample location at least at least in relation to the optical axis. Related systems and apparatus are also disclosed.