Mask-modulated spectra are incident to a sensor and are summed during a frame time. After the frame time, a compressed spectrum is read out based on the sum and decompressed to obtain spectra for some or all specimen locations. The mask-modulated spectrum that are summed are associated with different modulations produced by a common mask.

Even when the amount of overlay deviation between patterns located in different layers is large, correct measurement of the amount of overlay deviation is stably performed. The charged particle beam device includes a charged particle beam irradiation unit that irradiates a sample with a charged particle beam, a first detection unit that detects secondary electrons from the sample, a second detection unit that detects backscattered electrons from the sample, and an image processing unit that generates a first image including an image of a first pattern located on the surface of the sample based on an output of the first detection unit, and generates a second image including an image of a second pattern located in a lower layer than the surface of the sample based on an output of the second detection unit. A control unit adjusts the position of a measurement area in the first image based on a first template image for the first image, and adjusts the position of a measurement area in the second image based on a second template image for the second image.

A scanning electron microscope capable of properly determining a step of a step pattern formed on a sample regardless of combination of material of a groove of the step pattern and material of a projection of the step pattern, the scanning electron microscope includes a beam source, a detection unit having a first detection unit that detects a secondary electron emitted from the sample at an angle between an optical axis direction of the primary electron beam which is equal to or less than a predetermined value, and a second detection unit that detects a secondary electron emitted from the sample at an angle between the optical axis direction of the primary electron beam which is greater than the predetermined value, and a processing unit to obtain information on the step pattern using the information on a ratio between signals outputted from the first and the second detection unit.

A non-contact angle measuring apparatus includes a matter-wave and energy (MWE) particle source and a detector. The MWE particle source is used for generating boson or fermion particles. The detector is used for detecting a plurality peaks or valleys of an interference pattern generated by 1) the boson or fermion particles corresponding to a slit, a bump, or a hole of a first plane and 2) matter waves' wavefront-split associated with the boson or fermion particles reflected by a second plane, wherein angular locations of the plurality peaks or valleys of the interference pattern, a first distance between a joint region of the first plane and the second plane, and a second distance between the detector and the slit are used for deciding an angle between the first plane and the second plane.

An electron beam detection apparatus includes a first aperture element including a first set of apertures. The apparatus includes a second aperture element including a second set of apertures. The second set of apertures is arranged in a pattern corresponding with the pattern of the first plurality of apertures. The detection apparatus includes an electron-photon conversion element configured to receive electrons of the electron beam transmitted through the first and second aperture elements. The electron-photon conversion element is configured to generate photons in response to the received electrons. The detection apparatus includes an optical assembly including one or more optical elements. The detection apparatus includes a detector assembly. The optical elements of the optical assembly are configured to direct the generated photons from the electron-photon conversion system to the detector assembly.

To provide a technique capable of measuring high-frequency electrical noise in a charged particle beam device. A charged particle beam device 100 includes an electron source 2 for generating an electron beam EB1, a stage 4 for mounting a sample 10, a detector 5 for detecting secondary electrons EB2 emitted from the sample 10, and a control unit 7 electrically connected to the electron source 2, the stage 4, and the detector 5 and can control the electron source 2, the stage 4, and the detector 5. Here, when the sample 10 is mounted on the stage 4, and a specific portion 11 of the sample 10 is continuously irradiated with the electron beam EB1 from the electron source 2, the control unit 7 can calculate a time-series change in irradiation position of the electron beam EB1 based on an amount of the secondary electrons EB2 emitted from the specific portion 11, and can calculate a feature quantity for a shake of the electron beam EB1 based on the time-series change in irradiation position. Further, the feature quantity includes a frequency spectrum.

A method of determining a distortion of a field of view of a scanning electron microscope is described. The method may include: providing a sample including substantially parallel lines extending in a first direction; performing scans across the field of view of the sample along respective scan-trajectories extending in a scan direction; the scan direction being substantially perpendicular to the first direction; detecting a response signal of the sample caused by the scanning of the sample; determining a distance between a first line segment of a line and a second line segment of the line, whereby each of the first line segment and the second line segment are crossed by scan trajectories, based on the response signal; performing the previous step for multiple locations within the field of view; and determining the distortion across the field of view, based on the determined distances at the multiple locations.

A method for calibration including determining a temperature induced offset in a pedestal of a process module under a temperature condition for a process. The method includes delivering a wafer to the pedestal of the process module by a robot, and detecting an entry offset. The method includes rotating the wafer over the pedestal by an angle. The method includes removing the wafer from the pedestal by the robot and measuring an exit offset. The method includes determining a magnitude and direction of the temperature induced offset using the entry offset and exit offset.

A method of determining a distortion of a field of view of a scanning electron microscope is described. The method may include: providing a sample including substantially parallel lines extending in a first direction; performing scans across the field of view of the sample along respective scan-trajectories extending in a scan direction; the scan direction being substantially perpendicular to the first direction; detecting a response signal of the sample caused by the scanning of the sample; determining a distance between a first line segment of a line and a second line segment of the line, whereby each of the first line segment and the second line segment are crossed by scan trajectories, based on the response signal; performing the previous step for multiple locations within the field of view; and determining the distortion across the field of view, based on the determined distances at the multiple locations.

A method is provided of measuring the mass thickness of a target sample for use in electron microscopy. Reference data are obtained which is representative of the X-rays (28) generated within a reference sample (12) when a particle beam (7) is caused to impinge upon a region (14) of the reference sample (12). The region (14) is of a predetermined thickness of less than 300 nm and has a predetermined composition. The particle beam (7) is caused to impinge upon a region (18) of the target sample (16). The resulting X-rays (29) generated within the target sample (16) are monitored (27) so as to produce monitored data. Output data are then calculated based upon the monitored data and the reference data, the output data including the mass thickness of the region (18) of the target sample (16).