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.

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 decelerating electrode of this energy filter comprises: an electrode pair that has an opening; and a cavity portion that provided in a rotationally symmetrical manner with the center of the opening as the optical axis. Voltages with electric potentials that are substantially the same as that of a charged particle beam are independently applied to the both sides of the decelerating electrode. When an electrical field protrudes into the cavity portion provided in the decelerating electrode, a saddle point having the same electric potential as that of incident charged particles is formed inside the decelerating electrode. The saddle point acts as a high pass filter for incident charged particles at an energy resolution of 1 mV or less. By analyzing charged particles which have been energy-separated, it is possible to measure the energy spectrum and ΔE at the high resolution of 1 mV or less. In addition, by causing the energy-separated charged particle beam to converge and scan on the sample surface with an electron lens, it is possible to obtain an SEM/STEM image with a high resolution (see FIG. 3).

A charged particle beam apparatus covering a wide range of detection angles of charged particles emitted from a sample includes 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. The objective lens includes inner and outer magnetic paths which are formed so as to enclose a coil. A first inner magnetic path is disposed at a position opposite to an optical axis of the charged particle beams. A second inner magnetic path, formed at a slant with respect to the optical axis of the charged particle beams, includes a leading end. A detection surface of the detector is disposed at the outer side from a virtual straight line that passes through the leading end and that is parallel to the optical axis of the charged particle beams.

The disclosure relates to a method of imaging a specimen using a transmission charged particle microscope, said method comprising providing a specimen, and providing a charged particle beam and directing said charged particle beam onto said specimen for generating a flux of charged particles transmitted through the specimen. The method comprises the step of generating and recording a first energy filtered flux of charged particles transmitted through the specimen, wherein said first energy filtered flux of charged particles substantially consists of non-scattered and elastically scattered charged particles. The method as disclosed herein comprises the further step of generating and recording a second energy filtered flux of charged particles transmitted through the specimen, wherein said second energy filtered flux of charged particles substantially consists of inelastically scattered charged particles. Said first and second recorded energy filtered flux are then used for imaging said specimen with increased contrast.

The invention relates to a method of, and apparatus for, examining a sample using a charged particle beam apparatus. The method as defined herein comprises the step of detecting, using a first detector, emissions of a first type from the sample in response to the charged particle beam illuminating the sample. The method further comprises the step of acquiring spectral information on emissions of a second type from the sample in response to the charged particle beam illuminating the sample. As defined herein, said step of acquiring spectral information comprises the steps of providing a spectral information prediction algorithm and using said algorithm for predicting said spectral information based on detected emissions of the first type as an input parameter of said algorithm. With this it is possible to gather EDS data using only a BSE detector.

The invention relates to a method of examining a sample using a charged particle microscope, comprising the steps of providing a charged particle beam, as well as a sample; scanning said charged particle beam over said sample at a plurality of sample positions; and acquiring an EELS spectrum for each of said plurality of sample positions. According to the method, it comprises the further steps of scanning, once more, said charged particle beam over said sample at said plurality of sample positions; acquiring a further EELS spectrum for each of said plurality of sample positions; and combining, for each of said plurality of sample positions, said EELS spectrum with said further EELS spectrum. With this, it is possible to acquire rapid information on the sample being investigated, allowing for faster processing of samples.

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.

An apparatus for obtaining ion energy distribution, TED, measurements in a plasma processing system, in one example, comprising a substrate for placement in the plasma processing system and exposed to the plasma, an ion energy analyser disposed in the substrate for measuring the ion energy distribution at the substrate surface during plasma processing, the analyser comprising a first conductive grid, a second conductive grid, a third conductive grid, a fourth conductive grid, and a collection electrode, each grid separated by an insulation layer, a battery power supply and control circuitry, integrated in the substrate, for supplying and controlling voltage to each of the grids and the collector of the ion energy analyser; wherein at least one insulation layer includes a peripheral portion which is of reduced thickness with respect to the remaining portion of the insulation layer.

The invention relates to a method of, and apparatus for, examining a sample using a charged particle beam apparatus. The method as defined herein comprises the step of detecting, using a first detector, emissions of a first type from the sample in response to the charged particle beam illuminating the sample. The method further comprises the step of acquiring spectral information on emissions of a second type from the sample in response to the charged particle beam illuminating the sample. As defined herein, said step of acquiring spectral information comprises the steps of providing a spectral information prediction algorithm and using said algorithm for predicting said spectral information based on detected emissions of the first type as an input parameter of said algorithm. With this it is possible to gather EDS data using only a BSE detector.