Abstract:
A system for controlling a tool-to-tool disparity between a plurality of scanning electron microscopes includes a measuring unit for measuring a tool-to-tool disparity between plural scanning electron microscopes based on information extracted from secondary electron images which are captured by imaging a reference pattern formed on a wafer, a tool state monitoring unit for monitoring tool states of each of the plural scanning electron microscopes, and an output unit for displaying on a screen a relationship between the tool-to-tool disparity between the plural scanning electron microscopes and tool states of each of the plural scanning electron microscopes monitored by the tool state monitoring unit. The tool state monitoring unit monitors the tool states of each of the plural scanning electron microscopes while imaging the reference pattern formed on the wafer by using each of the plural scanning electron microscopes.
Abstract:
A method for measuring a demagnification of a charged particle beam exposure apparatus includes measuring a first stage position of a mask stage in accordance with a mask stage coordinate system, irradiating a first charged particle beam to a first irradiation position on a specimen through the opening portion of the mask, measuring the first irradiation position in accordance with a specimen stage coordinate system, moving the mask stage to a second stage position, measuring the second stage position of the mask stage, irradiating a second charged particle beam to a second irradiation position on the specimen through the opening portion of the mask measuring the second irradiation position in accordance with the specimen stage coordinate system, and calculating a demagnification of the charged particle beam exposure apparatus from the first and second stage positions and the first and second irradiation positions.
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:
A method for measuring a demagnification of a charged particle beam exposure apparatus includes measuring a first stage position of a mask stage in accordance with a mask stage coordinate system, irradiating a first charged particle beam to a first irradiation position on a specimen through the opening portion of the mask, measuring the first irradiation position in accordance with a specimen stage coordinate system, moving the mask stage to a second stage position, measuring the second stage position of the mask stage, irradiating a second charged particle beam to a second irradiation position on the specimen through the opening portion of the mask measuring the second irradiation position in accordance with the specimen stage coordinate system, and calculating a demagnification of the charged particle beam exposure apparatus from the first and second stage positions and the first and second irradiation positions.
Abstract:
In order to provide a full-automatic scanning electron microscope which carries out investigation jobs full-automatically from fine adjustment to reviewing, the scanning electron microscope of the present invention has a function of calculating the accuracy of correction after correction of coordinates and displaying it with vectors 39, a function of automatically determining a searching magnification for automatic object detection from the obtained information after correction of coordinates, and a function of calculating the frequency of occurrence of objects or defects and a time required for measurement from the searching magnification and conditions of measurement.
Abstract:
An electron beam apparatus for irradiating a target with an electron beam includes a reference sample including at least one reference pattern which has a plurality of lattice structures arranged along the circumference of a circle in a evaluation surface of the reference sample; and an adjustment section for adjusting the electron beam by irradiating the evaluation surface with the electron beam on the basis of electrons generated from the reference sample.
Abstract:
In an apparatus for measuring an intensity of an electron beam, the electron beam is made incident a fluorescent screen and a part of the incident electron beam is converted into an optical image, and the optical image formed on the fluorescent screen is picked-up by a television camera by a reflection mirror having a central hole and being inclined with respect to a direction into which the optical image is made incident upon the reflection mirror. A part of the electron beam transmitted through the fluorescent screen and passing through the central hole of the reflection mirror is made incident upon a Faraday case, which generates an electric current representing an intensity of the electron beam impinging upon the fluorescent screen. In the transmission type electron microscope, after measuring an intensity of the electron beam impinging upon the fluorescent screen, after removing the fluorescent screen, reflection mirror and Faraday cage from an optical axis, a shutter is opened to expose a photographic film to the electron beam for a time period which provides an optimum exposure on the basis of the measured intensity of the electron beam.
Abstract:
A tomographic technique for determining the power distribution of an electron beam using electron beam profile data acquired from a modified Faraday cup to create an image of the current density in high and low power beams. A refractory metal disk with a number of radially extending slits is placed above a Faraday cup. The beam is swept in a circular pattern so that its path crosses each slit in a perpendicular manner, thus acquiring all the data needed for a reconstruction in one circular sweep. Also, a single computer is used to generate the signals actuating the sweep, to acquire that data, and to do the reconstruction, thus reducing the time and equipment necessary to complete the process.
Abstract:
The present disclosure is related to a Schottky thermal field (TFE) source for emitting an electron beam. Electron optics can adjust a shape of the electron beam before the electron beam impacts a scintillator screen. Thereafter, the scintillator screen generates an emission image in the form of light. An emission image can be adjusted and captured by a camera sensor in a camera at a desired magnification to create a final image of the Schottky TFE source's tip. The final image can be displayed and analyzed to for defects.
Abstract:
An improved method and apparatus for enhancing an inspection image in a charged-particle beam inspection system. An improved method for enhancing an inspection image comprises acquiring a plurality of test images of a sample that are obtained at different landing energies, determining distortion levels for the plurality of test images, determining a landing energy level that enables the sample to be in a neutral charge condition during inspection based on the distortion levels, and acquiring an inspection image based on the determined landing energy level.