Abstract:
There is provided a method of adjusting a transmission electron microscope to facilitate an adjustment for bringing a focal plane of an electron beam exiting a two-stage filter type monochromator into coincidence with an achromatic plane. The method starts with obtaining a transmission electron microscope image including interference fringes of the electron beam that are generated by an aperture located behind the monochromator. The focal plane of the beam exiting the monochromator is brought into coincidence with the achromatic plane by adjusting the intensity of an electrostatic lens, the intensities of the electric and magnetic fields produced by at least one of two energy filters, or astigmatism generated in the monochromator based on an intensity distribution of the interference fringes in the obtained transmission electron microscope image.
Abstract:
Referring to design data for a sample, a measurement region is defined at a portion in the design data which has no step in an edge of a pattern. In addition, an edge as a characteristic portion is detected from the design data, and an edge as a characteristic portion corresponding to the characteristic portion of the design data is detected from a secondary electron image. Then, the measurement region is positioned and located in a secondary electron image based on a positional relationship between the edge of the design data and the edge of the secondary electron image. A width of the pattern is measured on the basis of a distance between the two edges included in the measurement region thus located.
Abstract:
A line-width measurement adjusting method, which is used when first and second electron beam intensity distributions for measuring a line width are produced from intensity distribution images of secondary electrons obtained respectively by scanning a first irradiation distance with an electron beam at first magnification, and by scanning a second irradiation distance with an electron beam at second magnification, includes the step of adjusting the second electron beam intensity distribution of the electron beam at the second magnification such that the second electron beam intensity distribution is equal to the first electron beam intensity distribution of the electron beam at first magnification. The second electron beam intensity distribution may be adjusted by increasing or decreasing a second irradiation distance when producing the electron beam intensity distribution.
Abstract:
Provided is a method for controlling electron beams in a multi-microcolumn, in which unit microcolumns having an electron emitter, a lens, and a deflector are arranged in an n×m matrix. A voltage is uniformly or differentially applied to each electron emitter or extractor. The same control voltage or different voltages are applied to a region at coordinates in a control division area of each extractor to deflect the electron beams. Lens layers not corresponding to the extractors are collectively or individually controlled so as to efficiently control the electron beams of the unit microcolumn. Further, a multi-microcolumn using the method is provided.
Abstract:
Provided is a charged particle beam processing apparatus capable of improving yields by suppressing the spread of metal pollution to a semiconductor manufacturing process to a minimum. The charged particle beam processing apparatus includes an ion beam column 1 that is connected to a vacuum vessel 10 and irradiates a sample 35 with an ion beam 11 of nonmetal ion species, a microsampling unit 3 having a probe 16 that extracts a microsample 43 cut out from a sample 35 by the ion beam 11, a gas gun 2 that discharges a gas for bonding the microsample 43 and the probe 16, a pollution measuring beam column 6A that is connected to the same vacuum vessel 10 to which the ion beam column 1 is connected and irradiates an ion beam irradiation traces by the ion beam column 1 with a pollution measuring beam 13, and a detector 7 that detects characteristic X-rays emitted from the ion beam irradiation traces by the ion beam column 1 upon irradiation with the pollution measuring beam 13.
Abstract:
An inspection apparatus and a semiconductor device manufacturing method using the same. The inspection apparatus is used for defect inspection, line width measurement, surface potential measurement or the like of a sample such as a wafer. In the inspection apparatus, a plurality of charged particles is delivered from a primary optical system to the sample, and secondary charged particles emitted from the sample are separated from the primary optical system and introduced through a secondary optical system to a detector. Irradiation of the charged particles is conducted while moving the sample. Irradiation spots of the charged particles are arranged by N rows along a moving direction of the sample and by M columns along a direction perpendicular thereto. Every row of the irradiation spots of the charged particles is shifted successively by a predetermined amount in a direction perpendicular to the moving direction of the sample.
Abstract:
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.
Abstract:
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.
Abstract:
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.
Abstract:
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.