The purpose of the present invention is to provide a defect inspection device that can evaluate a defect having a long latent flaw with high precision. A defect inspection device of the present invention is characterized by being provided with: a sample support member that supports a sample irradiated by an electron beam emitted from an electron source; an imaging element at which an image of electrons (mirror electrons) reflected without reaching the sample is formed via a retarding electric field formed on the sample; an ultraviolet light source that emits an ultraviolet light toward the sample; a movement stage that moves the sample support member; and a control device that controls the movement stage. The defect inspection device is further characterized in that the control device controls the movement stage such that a portion of a linear part included in an image of the sample (or a location on an extensional line of the linear part) is positioned at a specific location in an irradiated region of the electron beam, and repeats the control of the movement stage until an end of the linear part is positioned within the irradiated region of the electron beam.

A structure for grounding an extreme ultraviolet mask (EUV mask) is provided to discharge the EUV mask during the inspection by an electron beam inspection tool. The structure for grounding an EUV mask includes at least one grounding pin to contact conductive areas on the EUV mask, wherein the EUV mask may have further conductive layer on sidewalls or/and back side. The inspection quality of the EUV mask is enhanced by using the electron beam inspection system because the accumulated charging on the EUV mask is grounded. The reflective surface of the EUV mask on a continuously moving stage is scanned by using the electron beam simultaneously. The moving direction of the stage is perpendicular to the scanning direction of the electron beam.

A system for performing diffraction analysis, includes a mill for removing a surface portion of a sample, and an analyzer for performing diffraction analysis on the milled sample.

Systems and methods are disclosed that remove noise from roughness measurements to determine roughness of a feature in a pattern structure. In one embodiment, a method for determining roughness of a feature in a pattern structure includes generating, using an imaging device, a set of one or more images, each including measured linescan information that includes noise. The method also includes detecting edges of the features within the pattern structure of each image without filtering the images, generating a biased power spectral density (PSD) dataset representing feature geometry information corresponding to the edge detection measurements, evaluating a high-frequency portion of the biased PSD dataset to determine a noise model for predicting noise over all frequencies of the biased PSD dataset, and subtracting the noise predicted by the determined noise model from a biased roughness measure to obtain an unbiased roughness measure.

An improved charged particle beam inspection apparatus, and more particularly, a particle beam inspection apparatus including an improved alignment mechanism is disclosed. An improved charged particle beam inspection apparatus may include a second electron detection device to generate one or more images of one or more beam spots of the plurality of secondary electron beams during the alignment mode. The beam spot image may be used to determine the alignment characteristics of one or more of the plurality of secondary electron beams and adjust a configuration of a secondary electron projection system.

System and methods are described for directly measuring mechanical properties of a sample while concurrently imaging the sample using a scanning beam microscope (e.g., a scanning electron microscope (SEM)). The system includes a clamping mount configured to hold the sample and a load cell positioned proximal to the clamping mount and configured to provide a direct, real-time measurement of force on the sample end. The system further includes a controllable probe configured to apply a force to the sample. In some embodiments, the sample load cell is tiltably couplable to a sample held by the clamping mount and the controllable probe is moveable between a plurality of different mounting positions relative to the load cell.

There is provided a tilting parameters calculating device for use in a charged particle beam device for making a charged particle beam irradiated to a surface of a sample mounted on a sample stage, the tilting parameters calculating device being configured to calculate tilting parameters, the tilting parameters being input parameters to control a tilting direction and a tilting value of the sample and/or the charged particle beam, the input parameters being necessary to change an incident direction of the charged particle beam with respect to the sample, the tilting parameters calculating device including a tilting parameters calculating unit for calculating the tilting parameters based on information that indicates the incident direction of the charged particle beam with respect to a crystal lying at a selected position on the surface in a state where the incident direction of the charged particle beam with respect to the sample is in a predetermined incident direction, the information being designated on a crystal orientation figure, which is a diagram illustrating the incident direction of the charged particle beam with respect to a crystal coordinate system of the crystal.

A method and a charged particle beam system that includes charged particle beam optics and a movable stage; wherein the movable stage is configured to introduce a movement between the object and charged particle beam optics; wherein the movement is of a constant velocity and along a first direction; wherein the charged particle beam optics is configured to scan, by the charged particle beam, multiple areas of the object so that each point of the multiple areas is scanned multiple times; wherein the multiple areas partially overlap; wherein the scanning is executed by the charged particle beam optics; wherein the scanning comprises performing counter-movement deflections of the charged particle beam for at least partially compensating for the movement; and wherein each area of the multiple areas is scanned by following an area scan scheme that defines multiple scan lines that differ from each other.

Adjustable resolution electron energy loss spectroscopy methods and apparatus are disclosed herein. An example method includes operating an electron microscope in a first state, the first state including operating a source of the electron microscope at a first temperature, obtaining, by the electron microscope, a first EELS spectrum of a sample at a first resolution, the first resolution based on the first temperature, operating the electron microscope in a second state, the second state including operating the source of the electron microscope at a second temperature, the second temperature different than the first temperature, and obtaining, by the electron microscope, a second EELS spectrum of the sample at a second resolution, the second resolution based on the second temperature, wherein the second resolution is different than the first resolution.

Laser processing is enhanced by using endpointing or by using a charged particle beam together with a laser. End-pointing uses emissions, such as photons, electrons, ions, or neutral particles, from the substrate to determine when the material under the laser has changed or is about to change. Material removed from the sample can be deflected to avoid deposition onto the laser optics.