An electron microscope apparatus includes a detection unit that detects reflected electrons reflected from a sample when the sample is irradiated with primary electrons emitted by a primary electron generation unit (electron gun), an image generation unit that generates an image of a surface of the sample with the reflected electrons based on output from the detection unit, and a processing unit that generates a differential waveform signal of the image generated by the image generation unit, processes the image by using information of the differential waveform signal, and measures a dimension of a pattern formed on the sample.

A measurement device that comprises a photoelectric conversion element and a signal processing part that receives, from the photoelectric conversion element, detected pulses that include dark pulses and signal pulses that are outputted in accordance with inputted photons. The signal processing part performs amplitude discrimination on the detected pulses on the basis of a pre-acquired dark pulse amplitude distribution for the photoelectric conversion element.

An electron beam system for wafer inspection and review of 3D devices provides a depth of focus up to 20 microns. To inspect and review wafer surfaces or sub-micron-below surface defects with low landing energies in hundreds to thousands of electron Volts, a Wien-filter-free beam splitting optics with three magnetic deflectors can be used with an energy-boosting upper Wehnelt electrode to reduce spherical and chromatic aberration coefficients of the objective lens.

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.

An automatic detecting method and an automatic detecting apparatus using the same are provided. The automatic detecting apparatus includes an inputting unit, a dividing unit, a contouring unit, a range analyzing unit, a boundary analyzing unit, an edge detecting unit, an expanding unit and an overlapping unit. The dividing unit is used for dividing an overlooking image into four clusters via a clustering algorithm. The contouring unit is used for obtaining a contour. The range analyzing unit is used for obtaining a detecting range. The boundary analyzing unit is used for obtaining a circular boundary in the detecting range. The edge detecting unit is used for obtaining a plurality of edges in the circular boundary. The expanding unit is used for expanding the edges to obtain a plurality of expanded edges. The overlapping unit is used for overlapping the expanded edges and the contour to obtain a defect pattern.

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).

To improve detection efficiency of secondary particles without increasing a size of a charged particle beam apparatus, a charged particle beam apparatus according to the invention includes: a charged particle beam source configured to irradiate a sample with a primary particle beam; a scanning deflector configured to scan and deflect the primary particle beam to a desired position of the sample; and a detector configured to detect secondary particles emitted from the desired position. The charged particle beam apparatus further includes: a focusing lens electrode arranged coaxially with the primary particle beam and configured to generate a focusing electric field that is an electric field that focuses a trajectory of the secondary particles; and a mesh electrode configured to reduce leakage of the focusing electric field on a trajectory of the primary particle beam.

In the present invention, an electro-optical condition generation unit includes: a condition setting unit that sets, as a plurality of electro-optical conditions, a plurality of electro-optical conditions in which the combinations of the aperture angle and the focal-point height for an electron beam are different; an index calculating unit that determines a measurement-performance index in the electro-optical conditions set by the condition setting unit; and a condition deriving unit that derives an electro-optical condition, including an aperture angle and a focal-point height, so that the measurement-performance index determined by the index calculating unit becomes a prescribed value.

The methods and systems disclosed here detect edges of top-down images of respective cross-sections of an array of high-aspect-ratio (HAR) features. The respective cross sections are at various depths of a HAR feature along a longitudinal direction. The detected edges are re-sampled in a spatial domain at a target angular resolution. The re-sampled edges are represented as a corresponding set of harmonics in a frequency domain, each set of harmonics preserving characteristic information about a respective cross-section of the HAR feature at a certain depth. A plurality of cross-sections at the various depths of the HAR feature are reconstructed by analyzing the corresponding sets of harmonics in the frequency domain. A 3D profile of the HAR feature is generated by stitching the plurality of re-constructed cross-sections at the various depths of the HAR feature.