Patent application number | Description | Published |
20080197282 | Scanning Transmission Charged Particle Beam Device - There is provided a scanning transmission charged particle beam device by which charged particles of a bright-field image and charged particles of a dark-field image may be clearly separated, and bright-field images and dark-field images with high accuracy may be obtained even in a state in which the scanning range of a charged particle beams on a sample is changed. | 08-21-2008 |
20080224040 | Image Forming Method and Electron Microscope - As an image forming method including comparison between images for three-dimensional image construction or the like and an apparatus for forming such images, there are provided an image forming method and an electron microscope capable of obtaining with high accuracy or efficiency information required for comparison. In the image forming method, an image is formed on the basis of comparison between a plurality of images obtained by applying an electron beam to a specimen at different tilt angles. The method includes obtaining a first transmission image with the electron beam applied in a first direction and a second transmission image with the electron beam applied in a second direction, the second transmission image being formed within a region different from a peripheral blurred region resulting from tilting, and making a search in the first transmission image by using the second transmission image. | 09-18-2008 |
20090242792 | ELECTRON MICROSCOPY - Using, as a detector, a CCD detector having a CCD element to which a scintillator is closely fixed, a backscattered or scanning transmission image is obtained by the following method. The detector is disposed directly under an objective lens to obtain the backscattered electron image. When one point of a specimen is irradiated with an electron beam, backscattered or transmission electrons generated from the specimen collide with the scintillator to form a luminescent pattern. This pattern is detected by the CCD detector, and stored in a memory. This processing is sequentially repeated for each irradiation position to obtain all the patterns in an electron beam scanning range. Arithmetic processing is performed on each pattern to convert it into an image. Usually, image data for one pixel is calculated from one pattern. By sequentially repeating this, a backscattered or transmission electron image in the electronic beam scanning range can be obtained. | 10-01-2009 |
20090314938 | CHARGED PARTICLE BEAM APPARATUS AND DIMENSION MEASURING METHOD - There is provided a charged particle beam apparatus which allows implementation of a high-reliability and high-accuracy dimension measurement even if height differences exist on the surface of a sample. The charged particle beam apparatus includes the following configuration components: An acquisition unit for acquiring a plurality of SEM images whose focus widths are varied in correspondence with the focal depths, a determination unit for determining, from the plurality of SEM images acquired, a SEM image for which the image sharpness degree of the partial domain including a dimension-measuring domain becomes the maximum value, and a measurement unit for measuring the dimension of the predetermined domain from the SEM image whose image sharpness degree is the maximum value. | 12-24-2009 |
20130284923 | SCANNING ELECTRON MICROSCOPE - With a scanning electron microscope (SEM) adopting a commonly available exhaust system such as a turbo-molecular pump, an ion pump, or a rotary pump, and so forth, there is realized an apparatus capable of safely executing observation, or adsorption of a target substance that is high in rarity. Further, there is realized a safe SEM low in the risk of an electrical discharge by providing the apparatus with a probe, a means for replacing an atmosphere in a specimen chamber, with a predetermined gas, and a means for forming an image by detection of an ion current, and detection of an absorption current. Further, there is provided a means for controlling the polarity of a voltage applied to the probe. Still further, there is provided a control means for controlling a value of the voltage applied to the probe according to a degree of vacuum. | 10-31-2013 |