Various embodiments include measurement structures and methods for measuring integrated circuit (IC) images. In some cases, a measurement structure for use in measuring an image of an IC, includes: a first section having a positive shift spacing pattern; a second section, on an opposite side of the measurement structure, having a negative shift spacing pattern; and a third section having a reference spacing pattern for calibrating a measurement from at least one of the first section or the second section.

Various embodiments include measurement structures and methods for measuring integrated circuit (IC) images. In some cases, a measurement structure for use in measuring an image of an IC, includes: a first section having a positive shift spacing pattern; a second section, on an opposite side of the measurement structure, having a negative shift spacing pattern; and a third section having a reference spacing pattern for calibrating a measurement from at least one of the first section or the second section.

Disclosed are methods for sensing conditions of an electron microscope system and/or a specimen analyzed thereby. Also disclosed are sensor systems and electron microscope systems able to sense system conditions, and/or conditions of the specimen being analyzed by such systems. In one embodiment, a sparse dataset can be acquired from a random sub-sampling of the specimen by an electron beam probe of the electron microscope system. Instrument parameters, specimen characteristics, or both can be estimated from the sparse dataset.

Provided is a method for adjusting a field-of-view of a charged particle microscope device, in which reference data for a sample is set, a plurality of regions of interest are set for the reference data, a rough sampling coordinate group is set for each of the plurality of regions of interest, the sample is irradiated with charged particles based on the sampling coordinate group to obtain a corresponding pixel value group, a plurality of reconstructed images corresponding to the plurality of regions of interest are generated based on the pixel value group, a correspondence relationship among the plurality of regions of interest is estimated based on the plurality of reconstructed images, and the plurality of regions of interest are adjusted based on the correspondence relationship. Here, the sampling coordinate group is set based on the reference data.

In described examples, a method of operating a charged particle beam tool including a charged particle beam column configured to generate a charged particle beam includes capturing an under-focused image of a calibration target using the beam and capturing an over-focused image of the target using the beam. After determining an offset vector between the under-focused and over-focused images, if a magnitude of the offset vector is greater than a threshold, a charge distribution of the alignment electrodes is adjusted so that the charged particle beam has an adjusted alignment. The adjustment is made in response to the offset vector, to reduce a disalignment of the beam from an optical axis of the column. The method is then repeated using the adjusted alignment. If the magnitude of the offset vector is less than the threshold, the substrate is processed using the adjusted alignment.

An automatic method is provided to align a semiconductor crystalline substrate for electron channeling contrast imaging (ECCI) in regions where an electron channeling pattern cannot be reliably obtained but crystalline defects need to be imaged. The automatic semiconductor crystalline substrate alignment method is more reproducible and faster than the current operator intensive process for ECCI alignment routines. Also, the automatic semiconductor crystalline substrate alignment method increases the throughput of ECCI.

A device for detecting X-rays radiated out of a substrate surface, said device comprising at least one X-ray detector, a resolver grating and a modulator grating, said resolver grating with at least one opening facing towards said X-ray detector is arranged in front of said X-ray detector. Said modulator grating is provided between said resolver grating and said substrate at a predetermined distance from said resolver grating and said substrate, where said modulator grating having a plurality of openings in at least a first direction, wherein said x-rays from said surface is spatially modulated with said modulator grating and resolver grating.

The scanning charged particle beam microscope according to the present application is characterized in that, in acquiring an image of the FOV (field of view), interspaced beam irradiation points are set, and then, a deflector is controlled so that a charged particle beam scan is performed faster when the charged particle beam irradiates a position on the sample between each of the irradiation points than when the charged particle beam irradiates a position on the sample corresponding to each of the irradiation points (a position on the sample corresponding to each pixel detecting a signal). This allows the effects from a micro-domain electrification occurring within the FOV to be mitigated or controlled.

A method of producing a corrected beam of charged particles for use in a charged-particle microscope, comprising the following steps: Providing a non-monoenergetic input beam of charged particles; Passing said input beam through an optical module comprising a series arrangement of: A stigmator, thereby producing an astigmatism-compensated, energy-dispersed intermediate beam with a particular monoenergetic line focus direction; A beam selector, comprising a slit that is rotationally oriented so as to match a direction of the slit to said line focus direction, thereby producing an output beam comprising an energy-discriminated portion of said intermediate beam.

A device for detecting X-rays radiated out of a substrate surface, said device comprising at least one X-ray detector, a resolver grating and a modulator grating, said resolver grating with at least one opening facing towards said X-ray detector is arranged in front of said X-ray detector. Said modulator grating is provided between said resolver grating and said substrate at a predetermined distance from said resolver grating and said substrate, where said modulator grating having a plurality of openings in at least a first direction, wherein said x-rays from said surface is spatially modulated with said modulator grating and resolver grating.