A multi charged particle beam inspection apparatus includes a plurality of sensors, arranged inside or on a periphery of a secondary electron image acquisition mechanism, to measure a plurality of interfering factors, a determination circuit to determine, for each interfering factor, whether change exceeding a corresponding threshold is a first case which returns to the original state within a predetermined time period, or a second case which does not return to the original state even if the predetermined time period has passed, and a comparison circuit to input a reference image of a region corresponding to the secondary electron image acquired, and compare the secondary electron image with the reference image, wherein in the case where change of the second case occurs, the secondary electron image acquisition mechanism suspends the acquisition operation of the secondary electron image, and calibrates a change amount of the multiple charged particle beams.

The present invention enlarges a range of movement of field of view by beam deflection with a simple deflector configuration and suppresses deterioration of a signal electron detection rate caused by the beam deflection. A scanning electron microscope according to the present invention is provided with a first deflection field setting module that sets plural deflectors to move a scanning area on a specimen by a primary electron beam to a position deviated from an axis extended from an electron source toward the center of an objective lens and a second deflection field setting module that sets the plural deflectors so that trajectories of signal electrons are corrected without changing the scanning area set by the first deflection field setting module. The control unit controls the plural deflectors by adding a setting value set by the second deflection field setting module to a setting value set by the first deflection field setting module.

A multi charged particle beam inspection apparatus includes a plurality of sensors, arranged inside or on a periphery of a secondary electron image acquisition mechanism, to measure a plurality of interfering factors, a determination circuit to determine, for each interfering factor, whether change exceeding a corresponding threshold is a first case which returns to the original state within a predetermined time period, or a second case which does not return to the original state even if the predetermined time period has passed, and a comparison circuit to input a reference image of a region corresponding to the secondary electron image acquired, and compare the secondary electron image with the reference image, wherein in the case where change of the second case occurs, the secondary electron image acquisition mechanism suspends the acquisition operation of the secondary electron image, and calibrates a change amount of the multiple charged particle beams.

A method for generating cross-sectional profiles using a scanning electron microscope (SEM) includes scanning a sample with an electron beam to gather an energy-dispersive X-ray spectroscopy (EDS) spectrum for an energy level to determine element composition across an area of interest. A mesh is generated to locate positions where a depth profile will be taken. EDS spectra are gathered for energy levels at mesh locations. A number of layers of the sample are determined by distinguishing differences in chemical composition between depths as beam energies are stepped through. A depth profile is generated for the area of interest by compiling the number of layers and the element composition across the mesh.

A method for generating cross-sectional profiles using a scanning electron microscope (SEM) includes scanning a sample with an electron beam to gather an energy-dispersive X-ray spectroscopy (EDS) spectrum for an energy level to determine element composition across an area of interest. A mesh is generated to locate positions where a depth profile will be taken. EDS spectra are gathered for energy levels at mesh locations. A number of layers of the sample are determined by distinguishing differences in chemical composition between depths as beam energies are stepped through. A depth profile is generated for the area of interest by compiling the number of layers and the element composition across the mesh.

An ion implanter includes an energy analyzer electromagnet provided between an ion source and a processing chamber. The energy analyzer electromagnet includes a Hall probe configured to generate a measurement output in response to a deflecting magnetic field and an NMR probe configured to generate an NMR output. A control unit of the ion implanter includes a magnetic field measurement unit configured to measure the deflecting magnetic field in accordance with a known correspondence between the deflecting magnetic field and the measurement output, a magnetic field determination unit configured to determine the deflecting magnetic field from the NMR output, and a Hall probe calibration unit configured to update the known correspondence by using the deflecting magnetic field determined from the NMR output and a new measurement output of the Hall probe corresponding to the determined deflecting magnetic field.

A method for generating cross-sectional profiles using a scanning electron microscope (SEM) includes scanning a sample with an electron beam to gather an energy-dispersive X-ray spectroscopy (EDS) spectrum for an energy level to determine element composition across an area of interest. A mesh is generated to locate positions where a depth profile will be taken. EDS spectra are gathered for energy levels at mesh locations. A number of layers of the sample are determined by distinguishing differences in chemical composition between depths as beam energies are stepped through. A depth profile is generated for the area of interest by compiling the number of layers and the element composition across the mesh.

A method for generating cross-sectional profiles using a scanning electron microscope (SEM) includes scanning a sample with an electron beam to gather an energy-dispersive X-ray spectroscopy (EDS) spectrum for an energy level to determine element composition across an area of interest. A mesh is generated to locate positions where a depth profile will be taken. EDS spectra are gathered for energy levels at mesh locations. A number of layers of the sample are determined by distinguishing differences in chemical composition between depths as beam energies are stepped through. A depth profile is generated for the area of interest by compiling the number of layers and the element composition across the mesh.

The objective of the present invention is to provide a charged particle beam device, wherein the positional relationship between reflected electron detection elements and a sample and the vacuum state of the sample surroundings are evaluated to select automatically a reflected electron detection element appropriate for acquiring an intended image. In this charged particle beam device, all the reflected electron detection elements are selected when the degree of vacuum inside the sample chamber is high and the sample is distant from the reflected electron detectors, while a reflected electron detection element appropriate for acquiring a compositional image or a height map image is selected when the degree of vacuum inside the sample chamber is high and the sample is close to the reflected electron detectors. When the degree of vacuum inside the sample chamber is low, all the reflected electron detection elements are selected.

A method for generating cross-sectional profiles using a scanning electron microscope (SEM) includes scanning a sample with an electron beam to gather an energy-dispersive X-ray spectroscopy (EDS) spectrum for an energy level to determine element composition across an area of interest. A mesh is generated to locate positions where a depth profile will be taken. EDS spectra are gathered for energy levels at mesh locations. A number of layers of the sample are determined by distinguishing differences in chemical composition between depths as beam energies are stepped through. A depth profile is generated for the area of interest by compiling the number of layers and the element composition across the mesh.