Abstract:
It is an object of the present invention to obtain an image which is focused on all portions of a sample and to provide a charged particle beam apparatus capable of obtaining a two-dimensional image which has no blurred part over an entire sample. In order to achieve the above object, the present invention comprises means for changing a focus of a charged particle beam emitted from a charged particle source, a charged particle detector for detecting charged particles obtained at a portion of said sample irradiated with the charged particle beam, and means for composing a two-dimensional image of the sample as viewed from a direction of said charged particle beam source, based on signals on which said charged particle beam is focused, said signals being among signals output from the charged particle detector.
Abstract:
Secondary electrons emitted by a sample placed within a lens magnetic field are detected by a plurality of secondary electron detectors to enable observation of a concave/convex sample surface. In a scanning electronic beam apparatus having upper and lower electrodes built in a single-pole magnetic-field type lens to place a sample within a lens magnetic field, a negative voltage is applied to the sample and the lower electrode opposed thereto while a zero or positive voltage is applied to the upper electrode, whereby an electric field for suppressing the helical motion of a secondary electron given off from the sample due to electron-beam irradiation is produced within an objective magnetic field space above the sample. The secondary electrons are detected by a division-type MCP or a plurality of scintillator-type secondary electron detectors sandwiching the optical axis.
Abstract:
The secondary electrons, from a sample placed within a lens magnetic field, are detected by a plurality of secondary electron detectors, thereby effectively observing a concave/convex in a sample surface. In a scanning electronic beam apparatus having upper and lower electrodes built in a single-pole magnetic-field type lens to place a sample within a lens magnetic field, a negative voltage is applied to the sample and the lower electrode opposed thereto while a zero or positive voltage is applied to the upper electrode, whereby an electric field for suppressing the helical motion of a secondary electron given off from the sample due to electron-beam irradiation is caused within a region of from the sample to an objective lens magnetic field space closer to an electron source. The secondary electron is detected by a division-type MCP or a plurality of scintillator-type secondary electron detectors arranged sandwiching the optical axis.
Abstract:
An electron beam which can transmit through part of a specimen and can reach a portion not exposing to the electron beam is irradiated and a scanning image is obtained on the basis of a signal secondarily generated from a portion irradiated with the electron beam. Dimension-measuring start and end points are set on the scanning image and a dimension therebetween is measured. A cubic model is assumed, the cubic model is modified so as to match the scanning image, and dimension measurement is carried out on the basis of a modified cubic model.
Abstract:
A scanning electron microscope suitable for producing an image of high resolution by detecting secondary electrons and backscattered electrons generated from a specimen at a low accelerating voltage in a separate or synthesis fashion. In the scanning electron microscope electric and magnetic fields for separating trajectories of backscattered electrons and secondary electrons generated from a specimen are established, and a backscattered electron detector for detecting generated backscattered electrons is disposed on the trajectory of the backscattered electrons. According to the microscope, since secondary electrons and backscattered electrons can be detected efficiently in a separate fashion even at a low accelerating voltage of several kilovolts or less and besides the detector does not exert the deflection action on a primary electron beam, backscattered and secondary electron images of high resolution can be obtained.
Abstract:
An arrangement for observing a surface using a charged particle beam irradiated on the surface of a specimen and detecting secondary electrons emitted. An exciting device produces a strong magnetic field substantially perpendicular to the surface of the specimen. Secondary electrons are extracted from a bottom or side surface of a recess, such as a through hole formed in the surface of the specimen, by an interaction between the emitted secondary electrons and the strong magnetic field. A focusing lens is arranged so as to focus the charged particles at a point on the specimen, even in the presence of a strong field. Thus, a secondary electron image on the surface of the specimen can be sharply obtained to thereby observe a secondary electron image at the bottom surface or side surface of the through hole.
Abstract:
An object of the invention is to provide a charged particle beam apparatus which can perform optimized adjustment of a focusing condition of a charged particle beam focused on a sample and optimized adjustment of an orbit of a charged particle emitted from the sample. In order to achieve the above-described object, there is provided a charged particle beam apparatus including a passage restriction member that partially restricts passage of a charged particle emitted from a sample, a first lens that is arranged between the passage restriction member and the sample, and that controls an orbit of the charged particle emitted from the sample, and a second lens that is arranged between the passage restriction member and the charged particle source, and that changes a focusing condition of the charged particle beam in accordance with a control condition of the first lens.
Abstract:
A system that may include a processor, wherein the processor comprise an image waveform finder, a synthetic image generator and an output image generator; wherein the processor is configured to (i) receive or generate multiple images of a region of the object; wherein the region has an electron yield that is below an electron yield threshold; wherein each image is generated by scanning the region with an electron beam; (ii) process the multiple images to generate multiple synthetic images, and (iii) generate an output image of the region in response to the multiple synthetic images; wherein the image waveform finder is configured to process each image of the multiple images to find at least one image waveform that has a peak intensity that exceeds an intensity threshold; wherein the synthetic image generator is configured to replace one or more of the at least one image waveforms by one or more corresponding synthetic waveforms to provide a synthetic image; and wherein the output image generator is configured to generate an output image of the region in response to the multiple synthetic images
Abstract:
A system, method and a non-transitory compute readable medium for evaluating a high aspect ratio (HAR) hole having a nanometric scale width and formed in a substrate, including obtaining, during an illumination period, multiple measurement results by an electrostatic measurement device that comprises a probe tip that is placed in proximity to the HAR hole; wherein multiple locations within the HAR hole are illuminated with a beam of charged particles during the illumination period; and processing the multiple measurement results to determine a state of the HAR hole.
Abstract:
A sample observation device of the invention includes: a charged particle optical column for irradiating a sample with charged particle beams at a first acceleration voltage, the sample having a target part to be observed which is a concave part; an image acquisition part for acquiring an image including the target part to be observed on the basis of signals obtained by irradiation with the charged particle beams; a memory part for memorizing in advance, at each of a plurality of acceleration voltages, information indicating a relationship between a brightness ratio of a concave part to a periphery part of the concave part in a standard sample and a value indicating a structure of the concave part in the standard sample; and an operation part for obtaining a brightness ratio of the concave part to a periphery part of the concave part in the image. The operation part judges appropriateness/inappropriateness of the first acceleration voltage with the use of the information indicating the relationship and the brightness ratio in the image.