A scintillator assembly including an entrance surface for receiving charged particles into the scintillator assembly, the charged particles including first charged particles at a first energy level and second charged particles at a second energy level. A first scintillator structure configured for receiving the first charged particles and generating a corresponding first signal formed of first photons with a first wavelength of λ1, a second scintillator structure configured for receiving the second charged particles and generating a corresponding second signal of second photons with a second wavelength of λ2, and an emitting surface for egress of a combined signal from the scintillator assembly, the combined signal including the first and second photons, and at least one beam splitter for receiving the combined signal and separating the combined signal to first and second photons.

An apparatus and method are disclosed for monitoring and/or detecting concentrations of a chemical precursor in a reaction chamber. The apparatus and method have an advantage of operating in a high temperature environment. An optical emissions spectrometer (OES) is coupled to a gas source, such as a solid source vessel, in order to monitor or detect an output of the chemical precursor to the reaction chamber. Alternatively, a small sample of precursor can be periodically monitored flowing into the OES and into a vacuum pump, thus bypassing the reaction chamber.

An electron spectrometer is provided which can collect spectra in a reduced measurement time. The electron spectrometer includes an electron analyzer for providing energy dispersion of electrons emitted from a sample (S), a detector having a plurality of detection elements juxtaposed and arranged in the direction of energy dispersion of the dispersed electrons, and a processor. The processor operates (i) to sweep a measurement energy in first incremental energy steps (E.sub.1) within the analyzer, to detect the dispersed electrons with the detection elements, and to obtain a plurality of resulting first spectra; (ii) to interpolate points of measurement in each of the first spectra; and (iii) to generate a spectral chart in second incremental energy steps (E.sub.2) smaller than the first incremental energy steps (E.sub.1) on the basis of the first spectra for which the points of measurement have been interpolated.

A system and method are disclosed for acquiring Electron Energy Loss Spectrometry (EELS) spectra in a transmission electron microscope. The inventive system and method maximize spectrum acquisition rate and duty cycle by exposing a first portion of an image sensor to a first spectrum while a previously exposed potion of the sensor is read out of the sensor during some or all of the exposure time.

The present invention discloses an imaging device, an imaging method, and an imaging system, belonging to the field of sample image data acquisition and imaging technology. The imaging device includes: a charged particle source, a convergence system, a scanning control system, a detection module, and a spectral analysis module disposed below the detection module, where the detection module includes a plurality of pixelated detector units; and the detection module is provided with a hole thereon. The diffraction pattern is obtained by using the detection module, and the spectral analysis module performs spectral analysis on a charged particle beam passing through the hole, so as to obtain the diffraction pattern and spectral signal simultaneously by one scanning. The imaging method of the present invention is based on a hollow ptychography method, which enables toper form imaging on the diffraction pattern obtained through the detection module, with good imaging effects.

The purpose of the present invention is to provide a charged-particle beam device capable of stable performance of processes such as a measurement or test, independent of fluctuations in sample electric electric potential or the like. To this end, this charged-particle beam device comprises an energy filter for filtering the energy of charged particles released from the sample and a deflector for deflecting the charged particles released from the sample toward the energy filter. A control device generates a first image on the basis of the output of a detector, adjusts the voltage applied to the energy filter so that the first image reaches a prescribed state, and calculates deflection conditions for the deflector on the basis of the post-adjustment voltage applied to the energy filter.

A system, computer program product and a method for detecting manufacturing process defects, the method may include: obtaining multiple edge measurements of one or more structural elements after a completion of each one of multiple manufacturing phases; generating spatial spectrums, based on the multiple edge measurements, for each one of the multiple manufacturing phases; determining relationships between bands of the spatial spectrums; and identifying at least one of the manufacturing process defects based on the relationships between the bands of the spatial spectrums.

A scanning electron microscope having a spectrometer with a sensor having a plurality of pixels, wherein the spectrometer directs different wavelengths of collected light onto different pixels. An optical model is formed and an error function is minimized to find values for the model, such that wavelength detection may be corrected using the model. The model can correct for errors generated by effects such as the motion of the electron beam over the specimen, aberrations introduced by optical elements, and imperfections of the optical elements. A correction function may also be employed to account for effects not captured by the optical model.

A charged particle beam device includes: a charged particle beam source; an analyzer that analyzes and detects particles including secondary electrons and backscattered charged particles that are emitted from a specimen by irradiating the specimen with a primary charged particle beam emitted from the charged particle beam source; a bias voltage applying unit that applies a bias voltage to the specimen; and an analysis unit that extracts a signal component of the secondary electrons based on a first spectrum obtained by detecting the particles with the analyzer in a state where a first bias voltage is applied to the specimen, and a second spectrum obtained by detecting the particles with the analyzer in a state where a second bias voltage different from the first bias voltage is applied to the specimen.

Various methods and systems are provided for generating an energy resolved chroma image of a sample. Upon irradiated by a charged particle beam, scattered charged particles from the sample are directed to form a first image before entering a spectrometer. The scattered charged particles are then dispersed based on their energy when passing through the spectrometer. The dispersed particles form a second image on a detector. The scattered particles at each location of the first image is spread along a corresponding energy spread vector in the second image.