Abstract:
The present invention provides a scanning charged particle beam device including a sample chamber (8) and a detector. The detector has: a function of detecting light at least ranging from the vacuum ultraviolet region to the visible light region, of light (17) having image information which is obtained by a light emission phenomenon of gas scintillation when the sample chamber is controlled to a low vacuum (1 Pa to 3,000 Pa); and a function of detecting ion currents (11, 13) having image information which are obtained by cascade amplification of electrons and gas molecules. Accordingly, it becomes possible to realize a device which can deal with observation of various samples. Further, an optimal configuration of the detection unit is devised, to thereby make it possible to add value to an obtained image and provide users in wide-ranging fields with the observation image. In addition, the detector is made usable in combination with a detector for high vacuum, to thereby make it possible to provide wide-ranging users with the image, irrespective of the vacuum mode.
Abstract:
A high strength window for a radiation detection system has a plurality of ribs comprising beryllium material. There are openings between the plurality of ribs. The tops of the ribs terminate generally in a common plane. The high strength window also has a support frame around a perimeter of the ribs. A layer of thin polymer film material is disposed over and spans the plurality of ribs and openings to pass radiation therethrough. A radiation detection system comprises a high strength window as described above and a sensor behind the window. The sensor is configured to detect radiation that passes through the window.
Abstract:
A charged particle detector consists of four independent light guide modules assembled together to form a segmented on-axis annular detector, with a center opening for allowing the primary charged particle beam to pass through. One side of the assembly facing the specimen is coated with or bonded to scintillator material as the charged particle detection surface. Each light guide module is coupled to a photomultiplier tube to allow light signals transmitted through each light guide module to be amplified and processed separately. A charged particle detector is made from a single block of light guide material processed to have a cone shaped circular cutout from one face, terminating on the opposite face to an opening to allow the primary charged particle beam to pass through. The opposite face is coated with or bonded to scintillator material as the charged particle detection surface. The outer region of the light guide block is shaped into four separate light guide output channels and each light guide output channel is coupled to a photomultiplier tube to allow light signal output from each channel to be amplified and processed separately.
Abstract:
The present invention provides an electron microscope device, comprising a scanning electron microscope 2 provided with scanning means 10 for scanning an electron beam and an electron detector 12 for detecting an electron 11 issued from a specimen 8 where the electron beam is projected for scanning, wherein a scanning electron image is acquired based on a detection result from the electron detector, wherein the electron detector comprises a fluorescent substance layer for performing photoelectric conversion, a wavelength filter giving restriction so that all or almost all of wavelength ranges of fluorescent lights from the fluorescent substance layer can be transmitted, and a wavelength detecting element for receiving the fluorescent light transmitted through the wavelength filter and for performing photoelectric conversion.
Abstract:
An object of this invention is to make it easy to adjust a position of the energy beam to irradiate and a position of a focal point of a light collecting mirror part, and to prevent displacement of the light collecting part due to vibration with a simple arrangement. A sample measuring device in accordance with this invention is to measure light generated from a sample W by irradiating electron beams EB on the sample W, and comprises a electron optical column part 23 that converges the electron beams EB, and a light collecting mirror part 31 that is arranged between the electron optical column part 23 and the sample W and that has an energy beam path 312 to pass the electron beams EB converged by the electron optical column part 23 and to irradiate the electron beams EB on the sample W and a mirror face 311 whose focal point F is set on an axis of the energy beam path 312 and that collects the light L generated from the sample W by means of the mirror face 311, wherein the light collecting mirror part 31 is supported by the electron optical column part 23 so that the axis of the electron beams EB coincides with the focal point F.
Abstract:
According to an emission detecting analysis system and method, a test target is placed on a stage inside a chamber. A scanning electron microscope (SEM) column is installed at the chamber to obtain an image of the test target, and an emission detector column is installed at the chamber to detect light emission of the test target. High-magnification emission analysis and accurate detection of an emission point at a test target are obtained. In addition, a physical structure of the emission point is analyzed at the test target to reduce time required for analyzing a failure.
Abstract:
A method and apparatus for assessing a height of a specimen includes an electron beam unit having an electron beam source, lenses, a table for setting a specimen and controllable in a height direction, and a detector, and a height detection system for detecting height of the specimen set on the table while the specimen is irradiated by an electron beam. The height detection system further includes an illumination system, a collection system, first and second detectors, a device configured to receive output signals from the first and second detectors while the specimen is irradiated by the electron beam and to generate a comparison signal from the output signals, wherein the comparison signal is responsive to the height of the specimen.
Abstract:
An electron beam apparatus including a table which mounts a specimen and is movable in three dimensional directions, an electron beam optical system irradiating an electron beam onto a specimen and for detecting a secondary electron emanated from the specimen by the irradiation of the electron beam, and a surface height detection system for detecting height of the surface of the specimen mounted on the table. A focus control system controls a relative position between a focus position of the electron optical system and the table in accordance with information of the height, and an image processing system obtains an image from the detected secondary electron and processes the obtained image to detect a defect on the surface of the specimen.
Abstract:
A fiber optic plate assembly is provided for transferring optical signals to a detector or other optical element within an imaging device or imaging system. The fiber optic plate assembly comprises first and second fiber optic plates coupled via an optical coupling gel configured to permit separation of the two plates from each other to permit repair or replacement of one of the plates. Alternatively, the imaging device may comprise a single fiber optic plate coupled directly to an optical detector.
Abstract:
The present invention relates to an illuminant, etc., having a high response speed and a high luminous intensity. The illuminant comprises a substrate and a nitride semiconductor layer provided on one surface of the substrate. The nitride semiconductor layer emits fluorescence in response to incidence of electrons. At least part of the emitted fluorescence passes through the substrate, and then exits from the other surface of the substrate. Generation of the fluorescence is caused by incidence of electrons onto a quantum well structure of the nitride semiconductor layer and recombination of pairs of electrons and holes generated due to electron incidence, and the response speed of fluorescence generation is on the order of nanoseconds or less. Also, the luminous intensity of the fluorescence becomes equivalent to that of a conventional P47 fluorescent substance. Namely, the illuminant has a response speed and a luminous intensity that are sufficient for adaptation to scanning electron microscopes and mass spectroscopes.