A particle beam system includes a particle source to produce a first beam of charged particles. The particle beam system also includes a multiple beam producer to produce a plurality of partial beams from a first incident beam of charged particles. The partial beams are spaced apart spatially in a direction perpendicular to a propagation direction of the partial beams. The plurality of partial beams includes at least a first partial beam and a second partial beam. The particle beam system further includes an objective to focus incident partial beams in a first plane so that a first region, on which the first partial beam is incident in the first plane, is separated from a second region, on which a second partial beam is incident. The particle beam system also a detector system including a plurality of detection regions and a projective system.

The present invention provides a charged particle beam apparatus that covers a wide range of detection angles of charged particles emitted from a sample. Accordingly, the present invention proposes a charged particle beam apparatus that is provided with an objective lens for converging charged particle beams emitted from a charged particle source, and a detector for detecting charged particles emitted from a sample, wherein: the objective lens includes an inner magnetic path and an outer magnetic path which are formed so as to enclose a coil; the inner magnetic path comprises a first inner magnetic path disposed at a position opposite to an optical axis of the charged particle beams and a second inner magnetic path which is formed at a slant with respect to the optical axis of the charged particle beams and which includes a leading end of the magnetic path; and a detection surface of the detector is disposed at the outer side from a virtual straight line that passes through the leading end of the magnetic path and that is parallel to the optical axis of the charged particle beams.

A plurality of energy filter values are obtained using a model that simulates potential distribution within a 3D feature when an electron beam of an SEM impinges on a selected area that includes the 3D feature. A correspondence is extracted between the plurality of energy filter values and respective depths of the 3D feature along a longitudinal direction by analyzing the simulated potential distribution. A plurality of SEM images of the 3D feature corresponding to the plurality of energy filter values are obtained. The plurality of SEM images are associated with their respective depths based on the extracted correspondence between the plurality of energy filter values and the respective depths. A composite 3D profile of the 3D feature is generated from the plurality of SEM images obtained from various depths of the 3D feature.

A scanning electron microscopy system with improved image beam stability is disclosed. The system includes an electron beam source configured to generate an electron beam and a set of electron-optical elements to direct at least a portion of the electron beam onto a portion of the sample. The system includes an emittance analyzer assembly. The system includes a splitter element configured to direct at least a portion secondary electrons and/or backscattered electrons emitted by a surface of the sample to the emittance analyzer assembly. The emittance analyzer assembly is configured to image at least one of the secondary electrons and/or the backscattered electrons.

The invention relates to a transmission charged particle microscope comprising a charged particle beam source for emitting a charged particle beam, a sample holder for holding a sample, an illuminator for directing the charged particle beam emitted from the charged particle beam source onto the sample, and a control unit for controlling operations of the transmission charged particle microscope. As defined herein, the transmission charged particle microscope is arranged for operating in at least two modes that substantially yield a first magnification whilst keeping said diffraction pattern substantially in focus. Said at least two modes comprise a first mode having first settings of a final projector lens of a projecting system; and a second mode having second settings of said final projector lens.

The purpose of the present invention is to provide a charged particle ray device which is capable of simply estimating the cross-sectional shape of a pattern. The charged particle ray device according to the present invention acquires a detection signal for each different discrimination condition of an energy discriminator, and estimates the cross-sectional shape of a sample by comparing the detection signal for each discrimination condition with a reference pattern (see FIG. 5).

The invention is directed to mass spectrometer comprising an extraction system for secondary ions. The system comprises: an inner spherical deflecting sector; an outer spherical deflecting sector; a deflecting gap formed between the sectors; a housing in which the sectors are arranged. The deflecting sectors (42; 44) are biased at retarding gap (46). The system further comprises an exit disc electrode with an exit through hole centered about the exit axis, the intermediate electrode being biased at an intermediate voltage between the voltage of the housing and the average voltage of the sectors. The trajectories of the secondary ions become more parallel to the exit axis and become closer to the axis.

A semiconductor metrology tool for analyzing a sample is disclosed. The semiconductor metrology tool includes a particle generation system, a local electrode, a particle capture device, a position detector, and a processor. The particle generation system is configured to remove a particle from a sample. The local electrode is configured to produce an attractive electric field and to direct the removed particle towards an aperture of the local electrode. The particle capture device is configured to produce a repulsive electric field around a region between the sample and the local electrode and to repel the removed particle towards the aperture. The position detector is configured to determine two-dimensional position coordinates of the removed particle and a flight time of the removed particle. The processor is configured to identify the removed particle based on the flight time.

The present invention concerns an energy dispersion calibration method for calibrating an electron spectrometer of an electron spectrometer system including at least one electron emission source, electron optics and the electron spectrometer. The method comprising: obtaining, providing or receiving at least one electron energy loss spectrum produced by electrons of the electron spectrometer system exchanging energy with at least one resonant optical mode of an optical resonator into which light at a resonant wavelength is coupled; calculating or providing a Fourier transform of the at least one electron energy loss spectrum or a part of the at least one electron energy loss spectrum; determining or providing an energy dispersion (ΔE) of the electron spectrometer according to the equation

[00001]$\Delta E=f_E\frac{\mathrm{hc}}{\lambda N}\mathrm{or}\Delta E=f_E\frac{E_p}{N}.$

A particle beam system includes a particle source to produce a first beam of charged particles. The particle beam system also includes a multiple beam producer to produce a plurality of partial beams from a first incident beam of charged particles. The partial beams are spaced apart spatially in a direction perpendicular to a propagation direction of the partial beams. The plurality of partial beams includes at least a first partial beam and a second partial beam. The particle beam system further includes an objective to focus incident partial beams in a first plane so that a first region, on which the first partial beam is incident in the first plane, is separated from a second region, on which a second partial beam is incident. The particle beam system also a detector system including a plurality of detection regions and a projective system.