Methods and systems for performing sample lift-out and protective cap placement for highly reactive materials within charged particle microscopy systems are disclosed herein. Methods include preparing a nesting void in a support structure, translating at least a portion of a sample into the nesting void, and milling material from a region of the support structure that defines the nesting void. The material from the region of the support structure is milled such that at least some of the removed material redeposits to form an attachment bond between the sample and a remaining portion of the support structure. In various embodiments, the sample can then be investigated using one or more of serial sectioning tomography on the sample, enhanced insertable backscatter detector (CBS) analysis on the sample, and electron backscatter diffraction (EBSD) analysis on the sample.

A scanning electron microscopy system that includes a primary electron beam radiation unit configured to irradiate a first pattern of a substrate having a second pattern formed in a peripheral region of the first pattern, a detection unit configured to detect back scattered electrons emitted from the substrate, an image generation unit configured to generate an electron beam image corresponding to a strength of the back scattered electrons, a designating unit configured to designate a depth measurement region in which the first pattern exists on the electron beam image, and a processing unit configured to obtain an image signal of the depth measurement region and a pattern density in the peripheral region where the second pattern exists, and to estimate a depth of the first pattern based on the obtained image signal of the depth measurement region and the pattern density in the peripheral region.

Methods and apparatus determine offcut angle of a crystalline sample using electron channeling patterns (ECPs), wherein backscattered electron intensity exhibits angular variation dependent on crystal orientation. A zone axis normal to a given crystal plane follows a circle as the sample is azimuthally rotated. On an ECP image presented with tilt angles as axes, the radius of the circle is the offcut angle of the sample. Large offcut angles are determined by a tilt technique that brings the zone axis into the ECP field of view. ECPs are produced with a scanning electron beam and a monolithic backscattered electron detector; or alternatively with a stationary electron beam and a pixelated electron backscatter diffraction detector. Applications include strain engineering, process monitoring, detecting spatial variations, and incoming wafer inspection. Methods are 40× faster than X-ray diffraction. 0.01-0.1° accuracy enables semiconductor applications.

A detection and correction method for an electron beam system are provided. The method includes emitting an electron beam towards a specimen; modulating a beam current of the electron beam to obtain a beam signal. The method further includes detecting, using an electron detector, secondary and/or backscattered electrons emitted by the specimen to obtain electron data, wherein the electron data defines a detection signal. The method further includes determining, using a processor, a phase shift between the beam signal and the detection signal. The method further includes filtering, using the processor, the detection signal based on the phase shift.

A charged particle assessment tool including: an objective lens configured to project a plurality of charged particle beams onto a sample, the objective lens having a sample-facing surface defining a plurality of beam apertures through which respective ones of the charged particle beams are emitted toward the sample; and a plurality of capture electrodes, each capture electrode adjacent a respective one of the beam apertures, configured to capture charged particles emitted from the sample.

A wafer inspection system is disclosed. According to certain embodiments, the system includes an electron detector that includes circuitry to detect secondary electrons or backscattered electrons (SE/BSE) emitted from a wafer. The electron beam system also includes a current detector that includes circuitry to detect an electron-beam-induced current (EBIC) from the wafer. The electron beam system further includes a controller having one or more processors and a memory, the controller including circuitry to: acquire data regarding the SE/BSE; acquire data regarding the EBIC; and determine structural information of the wafer based on an evaluation of the SE/BSE data and the EBIC data.

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.

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.

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.

An object of the invention is to acquire a high-quality image while maintaining an improvement in throughput of image acquisition (measurement (length measurement)). The present disclosure provides a charged particle beam system including a charged particle beam device and a computer system configured to control the charged particle beam device. The charged particle beam device includes an objective lens, a sample stage, and a backscattered electron detector that is disposed between the objective lens and the sample stage and that adjusts a focus of a charged particle beam with which a sample is irradiated. The computer system adjusts a value of an electric field on the sample in accordance with a change in a voltage applied to the backscattered electron detector.