Abstract:
An electron microscope includes a secondary electron detector (51) which detects an electron generated when a sample (70) is illuminated with an electron beam from an electron gun (1), a monitor (39) which displays a secondary electron image of the sample based on an output of the detector, a gas inlet device (60) which emits gas to the sample, and a gas control device (81) which controls a gas emitting amount of the gas inlet device so that a degree of vacuum in an intermediate chamber (74) in which the secondary electron detector is installed may be kept at less than a set value P1 during gas emission performed by the gas inlet device. Accordingly, a microscopic image of the sample in a gas atmosphere with use of the detector requiring application of voltage is obtained.
Abstract:
The invention relates to an image capture assembly and method for use in an electron backscatter diffraction (EBSD) system. An image capture assembly comprises a scintillation screen (10) including a predefined screen region (11), an image sensor (20) comprising an array of photo sensors and a lens assembly (30). The image capture assembly is configured to operate in at least a first configuration or a second configuration. In the first configuration the lens assembly (30) projects the predefined region (11) of the scintillation screen (10) onto the array and in the second configuration the lens assembly (30) projects the predefined region (11) of the scintillation screen (10) onto a sub-region (21) of the array. In each of the first and second configurations the field of view of the lens assembly (30) is the same.
Abstract:
The disclosure relates to a low energy electron microscopy. The electron microscopy includes a vacuum chamber; an electron gun used to emit electron beam; a diffraction chamber; an imaging device; a sample holder used to fix two-dimensional nanomaterial sample; a vacuum pumping device; and a control computer. The electron beam transmits the sample to form a transmission electron beam and diffraction electron beam. The control computer includes a switching module to switch the work mode between a large beam spot diffraction imaging mode and small beam spot diffraction imaging mode.
Abstract:
Provided are a device and a method allowing a crystal orientation to be adjusted with adequate throughput and high precision to observe a sample, regardless of the type of the sample or the crystal orientation. In the present invention, the method comprises: setting a fitting circular pattern (26) displayed overlaid so that a main spot (23) is positioned on the circumference thereof, on the basis of the diffraction spot brightness distribution in an electron diffraction pattern (22b) displayed on a display unit (13); setting a vector (28) displayed with the starting point at the center position (27) of the displayed circular pattern (26), and the end point at the location of the main spot (23) positioned on the circumference of the circular pattern (26); and adjusting the crystal orientation on the basis of the orientation and the magnitude of the displayed vector (28).
Abstract:
A method of investigating a wavefront of a charged-particle beam that is directed from a source through an illuminator so as to traverse a sample plane and land upon a detector, an output of the detector being used in combination with a mathematical reconstruction technique so as to calculate at least one of phase information and amplitude information for the wavefront at a pre-defined location along its path to the detector, in which method: Said beam is caused to traverse a particle-optical lens system disposed between said sample plane and said detector; At a selected location in the path from said source to said detector, a modulator is used to locally produce a given modulation of the wavefront; In a series of measurement sessions, different such modulations are employed, and the associated detector outputs are collectively used in said mathematical reconstruction.
Abstract:
A system and method are provided for preparing and analyzing an object having a region of interest. Material is removed from a first surface of the object using a second particle beam. The first surface is monitored using a first particle beam and a second detector. A second surface of the object is generated when the material is removed from the first surface. Material is removed from the second surface using the second particle beam, and the removal of the material is monitored using the first particle beam and the second detector. Removing the material generates a first side and a second side, and the region of interest is arranged between the first side and the second side. The first particle beam is guided to the first side, and first charged particles of the first particle beam being transmitted through the region of interest are detected using a first detector.
Abstract:
There is a limit in range and distance in which an electron beam can interfere and electron interference is implemented within a range of a coherence length. Therefore, interference images are consecutively recorded for each interference region width from an interference image of a reference wave and an observation region adjacent to the reference wave by considering that a phase distribution regenerated and observed by an interference microscopy is a differential between phase distributions of two waves used for interference and a differential image between phase distributions of a predetermined observation region and a predetermined reference wave is acquired by acquiring integrating phase distributions acquired by individually regenerating the interference images. This work enables a wide range of interference image which is more than a coherence length by arranging phase distribution images performed and acquired in the respective phase distributions in a predetermined order.
Abstract:
In accordance with an embodiment, a sample structure analyzing method includes generating a beam and then applying the beam to a plurality of observation regions on a sample, and acquiring a plurality of diffraction images from the beam which has passed through the sample; and comparing the acquired diffraction images, and judging the difference between the observation regions from the comparison result, or identifying the grain boundary of crystal constituting the sample.
Abstract:
The present invention provides an on-chip thin film phase plate for a releasing charging, comprising a chip substrate having one or more apertures; and a thin film layer attached to the top surface of the chip substrate. The present invention also provides a method for observing organic material by TEM, which uses the above-mentioned on-chip thin film phase plate in a TEM system.
Abstract:
A charged particle beam system for performing precession diffraction includes a lens 11 for focusing a beam 5 in an object plane 9, and an objective lens 13 having a diffraction plane 27. A doublet 53 of lenses 35, 63 images the diffraction plane 27 into an intermediate diffraction plane 69 where a multipole 55 is located. A doublet 57 of lenses 65, 93 images the intermediate diffraction plane 69 into an intermediate diffraction plane 71 where a multipole 59 is located. A first deflection system 15 upstream of the object plane 9 can tilt to change an angle of incidence of the beam on the object plane. A second deflection system 37 between lenses 35 and 63 tilts the beam such that the change of the angle of incidence of the charged particle beam on the object plane is compensated.