Notches or chevrons with known angles relative to each other are formed on a surface of the sample, where each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

A multi-electron beam system that forms hundreds of beamlets can focus the beamlets, reduce Coulomb interaction effects, and improve resolutions of the beamlets. A Wien filter with electrostatic and magnetic deflection fields can separate the secondary electron beams from the 5 primary electron beams and can correct the astigmatism and source energy dispersion blurs for all the beamlets simultaneously.

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.

Provided is a projection electron beam application apparatus suitable for use in semiconductor manufacturing lines. An electron optical system of the electron beam application apparatus includes a mirror aberration corrector 106 disposed perpendicular to an optical axis 109, a plurality of magnetic field sectors 104 by which an orbit of electrons is deviated from the optical axis to make the electrons incident on the mirror aberration corrector 106, and the orbit of the electrons emitted from the mirror aberration corrector 106 is returned to the optical axis, and a doublet lens 105 disposed between adjacent magnetic field sectors along the orbit of the electrons. The plurality of magnetic field sectors have the same deflection angle for deflecting the orbit of the electrons, and the doublet lens is disposed such that an object plane and an image plane thereof are respectively central planes of the adjacent magnetic field sectors along the orbit of the electrons.

A multi-beam apparatus for multi-beam inspection with an improved source conversion unit providing more beamlets with high electric safety, mechanical availability and mechanical stabilization has been disclosed. The source-conversion unit comprises an image-forming element array having a plurality of image-forming elements, an aberration compensator array having a plurality of micro-compensators, and a pre-bending element array with a plurality of pre-bending micro-deflectors. In each of the arrays, adjacent elements are placed in different layers, and one element may comprise two or more sub-elements placed in different layers. The sub-elements of a micro-compensator may have different functions such as micro-lens and micro-stigmators.

A method of operating a multi-column electron beam array for quality inspection of a semiconductor wafer involves dividing the whole wafer area collectively in equally divided areas allocated to each column of the array, and assigning each of the areas as a column working space having the same dimensions and orientations. The array of column working spaces are assigned to an array of column optical axes, wherein a field of view of each column is defined as a covered region in which critical wafer patterns can be scanned by one or more columns to take an image. The stage supporting the wafer is moved such that each column working space is fully covered by the field of view of each column completely. By utilizing arbitrary waveform generators in electron inspection columns, this method also can be extended to write independent arbitrary patterns in predetermined positions in each die on a wafer.

A charged particle beam inspection method conducted by disposing a sample on a stage and by performing a first scanning in a first beam scanning area on the sample by using one first charged particle beam out of a plurality of charged particle beams while the stage is moved so that a first inspection of a first inspection unit in the first beam scanning area is performed, and by performing a second scanning in a second beam scanning area on the sample by using one second charged particle beam out of the charged particle beams while the stage is moved so that a second inspection of a second inspection unit in the second beam scanning area is performed.

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.

The present invention relates to a charged particle beam device capable of suppressing table deformation caused by movement of a rolling element of a guide with a simple configuration, and a strain isolation guide structure, a stage using the guide structure, and a charged particle beam device using the stage are proposed, the strain isolation guide structure being characterized in that, in a sample stage including a linear guide including a carriage (201), a rolling element, and a guide rail (202), and a table (105), the carriage (201) and the table (105) are connected via an adapter (401) as an elastically deformable member.

Linear fiducials with known angles relative to each other are formed such that their structures appear in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.