Abstract: The present invention relates to an electron microscope which reduces a difference in measured values that occur due to a difference in resolution that cannot be fully adjusted which exists among electron microscopes, or occurs as time elapses, and a method for measuring dimensions. An operator adapted to compensate for changes of an electron image to be generated due to a difference in probe diameter is obtained in advance from electron images of one reference sample created by electron microscopes having different resolution (probe diameter). Then a compensation-measurement electron image which is equivalent to an electron image created under the same probe diameter by applying the operator for compensation, and the compensation-measurement electron image is used for measuring the dimensions.

Abstract: In a scanning electron microscope, slimming is reduced by reducing a frame count. As the frame count is reduced, the amount of detected secondary electrons decreases, so that a probe current amount is increased to emit an increased amount of detected secondary electrons. A primary electron beam is scanned on a sample, a histogram is created, and the histogram is second-order differentiated to calculate a level of halftone at which a sample image changes in contrast, and to calculate the probe current amount. By adjusting the frame count suitable for the calculated probe current amount, and the contrast suitable for the sample image, the slimming of the sample is limited, and a highly visible sample image is generated for length measurement.

Abstract: Equipment extracts components of spatial frequency that need to be evaluated in manufacturing a device or in analyzing a material or process out of edge roughness on fine line patterns and displays them as indexes. The equipment acquires data of edge roughness over a sufficiently long area, integrates a components corresponding to a spatial frequency region being set on a power spectrum by the operator, and displays them on a length measuring SEM. Alternatively, the equipment divides the edge roughness data of the sufficiently long area, computes long-period roughness and short-period roughness that correspond to an arbitrary inspection area by performing statistical processing and fitting based on theoretical calculation, and displays them on the length measuring SEM.

Abstract: A calibration standard specimen is provided to have formed therein calibrating patterns of a lattice shape discontinuously arrayed, and particular alignment patterns respectively disposed near the calibrating patterns so that the positioning of the specimen can be made to match the calibrating patterns to the measurement points.

Abstract: In the case of monitoring a resolution of a scanning electron microscope, it is required to prepare a sample and to use a measuring algorithm so as to reduce the pattern dependency of an index value of resolution to be measured in order to measure a variation in the size of an electron beam with a high degree of accuracy. According to the present invention, there is used a sample having a sectional shape which is appropriate for monitoring the resolution, that is, the sample has a pattern with such a sectional shape that a side wall of the pattern is inclined so as to prevent an electron beam irradiated on the sample from impinging upon the side wall of the pattern. With this configuration, it is possible carry out such resolution monitor that does not depend upon a sectional shape of a pattern.

Abstract: A calibration standard specimen is provided to have formed therein calibrating patterns of a lattice shape discontinuously arrayed, and particular alignment patterns respectively disposed near the calibrating patterns so that the positioning of the specimen can be made to match the calibrating patterns to the measurement points.

Abstract: Disclosed is a scanning electron microscope (SEM) for realizing high-precision dimension measurement of a sample, such as an ArF exposure photoresist, that requires the measurement of a dimension by a low S/N signal waveform. To this end, partial waveforms (or partial images) of sample signal waveforms (or an images) acquired from a dimension measurement target sample and a sample material of the same kind are registered in advance, a measurement target signal waveform (or an image) obtained from the dimension measurement target sample and the sample registration waveform are combined, and a dimension of the dimension measurement target pattern is calculated based on the combination result.

Abstract: A scanning method for a scanning electron microscope is provided which minimizes a degradation in dimension measuring accuracy caused by a shrink of a specimen. A time between the first and the second scan over the same location on the specimen is shortened by changing the scanning order of scan lines to enable the scanning to be performed successively while the shrink is small.

Abstract: An object of the present invention is to suppress measurement errors caused by the fact that the shrink amount due to scan of an electron beam differs pattern by pattern. To accomplish this object, according to the invention, functions indicative of a process of change of pattern dimension when the electron beam is irradiated on a sample are prepared in respect of the kinds of sample patterns, and dimension values of a particular pattern measured by scanning the electron beam on the particular pattern are fitted to a function prepared for the particular pattern to calculate a dimension of the particular pattern before it changes.

Abstract: A quantity (or dispersion value) of a distribution of edge position due to random noise is expected to be reduced statistically to 1/N when N edge position data items are averaged. Using this property, the single page image is averaged in a vertical direction with various values of parameter S, and then the edge roughness index is calculated. The S-dependence of the edge roughness index is analyzed and a term of a dispersion value directly proportional to 1/S is determined as being due to noise.

Abstract: Disclosed is a scanning electron microscope (SEM) for realizing high-precision dimension measurement of a sample, such as an ArF exposure photoresist, that requires the measurement of a dimension by a low S/N signal waveform. To this end, partial waveforms (or partial images) of sample signal waveforms (or an images) acquired from a dimension measurement target sample and a sample material of the same kind are registered in advance, a measurement target signal waveform (or an image) obtained from the dimension measurement target sample and the sample registration waveform are combined, and a dimension of the dimension measurement target pattern is calculated based on the combination result.

Abstract: A focus adjustment method and a focus adjustment apparatus suited to realize both higher precision and faster speed of focus adjustment are provided. More specifically, the focus adjustment method and apparatus of this invention determine a focus adjustment quantity based on a relation between a change in a focus position value and a change in a focus evaluation value or a relation between the focus position value and the focus evaluation value, namely, a gradient of the focus evaluation value in a focus position direction. As one example, an excitation current to be supplied to an objective lens (or a voltage to be applied to a specimen) is calculated based on the relation between a change in the excitation current (or voltage applied to the specimen) and a change in the focus evaluation value.

Abstract: The present invention provides a charged particle beam apparatus used to measure micro-dimensions (CD value) of a semiconductor apparatus or the like which captures images for measurement. For the present invention, a sample for calibration, on which a plurality of polyhedral structural objects with known angles on surfaces produced by the crystal anisotropic etching technology are arranged in a viewing field, is used. A beam landing angle at each position within a viewing field is calculated based on geometric deformation on an image of each polyhedral structural object. Beam control parameters for equalizing the beam landing angle at each position within the viewing field are pre-registered. The registered beam control parameters are applied according to the position of the pattern to be measured within the viewing field when performing dimensional measurement.

Abstract: An image forming method and a charged particle beam apparatus suitable for suppressing the inclination of charging when scanning a two-dimensional area with a charged particle beam. A third scanning line located between a first scanning line and a second scanning line is scanned. After the first, second and third scanning lines have been scanned, a plurality of scanning lines are scanned between the first and third scanning lines and between the second and third scanning lines.

Abstract: A quantity (or dispersion value) of a distribution of edge position due to random noise is expected to be reduced statistically to 1/N when N edge position data items are averaged. Using this property, the single page image is averaged in a vertical direction with various values of parameter S, and then the edge roughness index is calculated. The S-dependence of the edge roughness index is analyzed and a term of a dispersion value directly proportional to 1/S is determined as being due to noise.

Abstract: A system for controlling a tool-to-tool matching between a plurality of scanning electron microscopes for pattern dimension measurement includes a measuring unit for, at regular intervals, measuring a tool-to-tool disparity between scanning electron microscopes based on secondary electron image data, and measuring indicators indicating states of the microscopes, a tool-to-tool-disparity causing factor analyzing unit for analyzing a relationship between the tool-to-tool disparity and the values of the indicators measured by the measuring unit to estimate a factor that has caused said tool-to-tool disparity, and an output unit for displaying and outputting the tool-to-tool disparity causing factor estimated by the tool-to-tool-disparity causing factor analyzing unit.

Abstract: Disclosed is a scanning electron microscope (SEM) for realizing high-precision dimension measurement of a sample, such as an ArF exposure photoresist, that requires the measurement of a dimension by a low S/N signal waveform. To this end, partial waveforms (or partial images) of sample signal waveforms (or an images) acquired from a dimension measurement target sample and a sample material of the same kind are registered in advance, a measurement target signal waveform (or an image) obtained from the dimension measurement target sample and the sample registration waveform are combined, and a dimension of the dimension measurement target pattern is calculated based on the combination result.

Abstract: According to the invention, to achieve the above objective, there is provided a charged particle beam apparatus that creates a first image by irradiating a charged particle beam on a sample to scan a first pattern of the sample, controls on the basis of the first image the focus of the charged particle beam and the brightness and/or contrast of the image, and irradiates the charged particle beam to correctly scan a second pattern different from the first pattern by using the control conditions used to control the focus of the charged particle beam and the brightness and/or contrast of the image.

Abstract: The SEM has a dynamic range reference value setting unit for setting dynamic range reference values, a dynamic range adjustment unit for receiving an observation image signal delivered out of a secondary electron detector, adjusting the dynamic range of the observation image signal on the basis of the dynamic range reference values and outputting the thus adjusted observation image signal as an observation image signal after adjustment, a display image generation unit for determining luminous intensity levels of individual pixels of an image to be displayed based on the observation image signal after adjustment to generate a display image, a histogram generation unit for generating a histogram of luminous intensity levels of the display image and extracting, as a luminous intensity peak value, at which the frequency of luminous intensity is maximized, and a display unit for displaying the generated histogram and the extracted luminous intensity peak value.

Abstract: An image forming method and a charged particle beam apparatus suitable for suppressing the inclination of charging when scanning a two-dimensional area with a charged particle beam. A third scanning line located between a first scanning line and a second scanning line is scanned. After the first, second and third scanning lines have been scanned, a plurality of scanning lines are scanned between the first and third scanning lines and between the second and third scanning lines.