Abstract:
Systems, methods, and components of charged particle microscopes affording improved contrast in dose sensitive samples are described. A pole piece for an electron microscope can include a body, being substantially concentric with a central axis. The body can define an upper surface, substantially normal to the central axis, a lower surface, substantially normal to the central axis, a central aperture formed in the body from the upper surface to the lower surface. The central aperture can be substantially rotationally symmetrical about the central axis. The body can define a lateral surface, inclined relative to the central axis and tapering toward the upper surface and a plurality of lateral apertures formed in the body from the lateral surface to the central aperture. The plurality of lateral apertures can be arrayed substantially symmetrically about the central axis.
Abstract:
Method and system for generating a diffraction image comprises acquiring multiple frames from a direct-detection detector responsive to irradiating a sample with an electron beam. Multiple diffraction peaks in the multiple frames are identified. A first dose rate of at least one diffraction peak in the identified diffraction peaks is estimated in the counting mode. If the first dose rate is not greater than a threshold dose rate, a diffraction image including the diffraction peak is generated by counting electron detection events. Values of pixels belonging to the diffraction peak are determined with a first set of counting parameter values corresponding to a first coincidence area. Values of pixels not belonging to any of the multiple diffraction peaks are determined using a second, set of counting parameter values corresponding to a second, different, coincidence area.
Abstract:
Diffraction patterns of a sample at various tilt angles are acquired by irradiating a region of interest using a first charged particle beam. Sample images are acquired by irradiating the region of interest using a second charged particle beam. The first and second charged particle beams are formed by splitting charged particles generated by a charged particle source.
Abstract:
Techniques of using a Transmission Charged Particle Microscope for diffraction pattern detection are disclosed. An example method including irradiating at least a portion of a specimen with a charged particle beam, using an imaging system to collect charged particles that traverse the specimen during said irradiation, and to direct them onto a detector configured to operate in a particle counting mode, using said detector to record a diffraction pattern of said irradiated portion of the specimen, recording said diffraction pattern iteratively in a series of successive detection frames, and during recording of each frame, using a scanning assembly for causing relative motion of said diffraction pattern and said detector, so as to cause each local intensity maximum in said pattern to trace out a locus on said detector.
Abstract:
A method of investigating a specimen using X-ray tomography, comprising (a) mounting the specimen to a specimen holder, (b) irradiating the specimen with a beam of X-rays along a first line of sight through the specimen, and (c) detecting a flux of X-rays transmitted through the specimen and forming a first image. Then (d) repeating the steps (b) and (c) for a series of different lines of sight through the specimen, thereby producing a corresponding series of images. The method further comprises (e) performing a mathematical reconstruction on said series of images, so as produce a tomogram of at least part of the specimen, wherein the specimen is disposed within a substantially cylindrical metallic shell with an associated cylindrical axis, the beam of X-rays is produced by directing a beam of charged particles onto a zone of said metallic shell, so as to produce a confined X-ray source at said zone, and the series of different lines of sight is achieved by rotating said shell about said cylindrical axis, thereby causing relative motion of said zone relative to the specimen.
Abstract:
The invention relates to a method of inspecting parts of a sample on a TEM grid with a fluorescence microscope, as arises when performing correlative microscopy, more specifically for samples on a holey carbon grid. A problem occurs when imaging vitrified ice with sample material when the ice is heated by the light used. The invention is based on the insight that the absorption in the carbon support film is responsible for the heating, as ice hardly absorbs light. By localizing the illumination of the fluorescent microscope to the parts of the sample that are above a hole in the carbon, heating of the ice is lowered. The localization can be achieved by, for example, passing the light through a LCD type Spatial Light Modulator.
Abstract:
Molecular structure may be determined based on structure factors solved from the diffraction pattern and the electron microscopy image of the sample. In particular, the amplitudes of the structure factors may be determined based on intensities of diffraction peaks in the multiple diffraction patterns. The phases of the structure factors may be determined based on electron microscopy images and the intensities of the diffraction peaks.
Abstract:
An x-ray source for computer tomography uses several sub-sources. An electron beam impacts the several sub-sources to achieve a high x-ray flux with high resolution. The several sub-sources produce a composite image, which is deconvolved to disentangle the composite image and render a useful image. The configuration of the several sub-sources can be optimized for a given specimen structure.
Abstract:
Examining a sample in a charged-particle microscope of a scanning transmission type includes: Providing a beam of charged particles that is directed from a source through an illuminator so as to irradiate the sample; Providing a detector for detecting a flux of charged particles traversing the sample; Causing said beam to scan across a surface of the sample, and recording an output of the detector as a function of scan position, resulting in accumulation of a charged-particle image of the sample, Embodying the detector to comprise a plurality of detection segments; Combining signals from different segments of the detector so as to produce a vector output from the detector at each scan position, and compiling this data to yield a vector field; and Mathematically processing said vector field by subjecting it to a two-dimensional integration operation, thereby producing an integrated vector field image.
Abstract:
A Correlative Light and Electron Microscope (CLEM) is equipped with a TEM column and a light microscope fitted between the pole shoes of the objective lens of the TEM. To enlarge the acceptance solid angle for enhanced sensitivity a truncated lens is used. It is noted that this does not imply that the lens shows astigmatism (it is not a cylindrical lens).Using the light microscope, a first image is made with the sample in a first direction. This image will show in one direction a higher (diffraction limited) resolution than in the direction perpendicular thereto, due to the different NA of the lens in the two directions. By rotating the sample and making a second image, a combined image can be formed showing a better resolution than either of the images in the direction where they show a low NA.