Abstract:
A user interface for operation of a scanning electron microscope device that combines lower magnification reference images and higher magnification images on the same screen to make it easier for a user who is not used to the high magnification of electron microscopes to readily determine where on the sample an image is being obtained and to understand the relationship between that image and the rest of the sample. Additionally, other screens, such as, for example, an archive screen and a settings screen allow the user to compare saved images and adjust the settings of the system, respectively.
Abstract:
When preparing a Hole-Free Phase Plates (HFPP) a preferably featureless thin film should be placed with high accuracy in the diffraction plane of the TEM, or a plane conjugate to it. Two methods for accurately placing the thin film in said plane are described. One method uses a Ronchigram of the thin film while the TEM is in imaging mode, and the magnification of the Ronchigram is tuned so that the magnification in the middle of the Ronchigram is infinite. The second method uses electrons scattered by the thin film while the TEM is in diffraction mode. When the thin film does not coincide with the diffraction plane, electrons scattered by the thin film seem to originate from another location than the cross-over of the zero beam. This is observed as a halo. The absence of the halo is proof that the thin film coincides with the diffraction plane.
Abstract:
A freestanding thin film of nano-crystalline graphite is described, as well as a method of producing a freestanding thin film of nano-crystalline graphite including: providing a freestanding thin film of amorphous carbon, heating the freestanding thin film to a high temperature in an inert atmosphere or in a vacuum; and allowing the freestanding thin film to cool down, as a result of which a freestanding thin film of nano-crystalline graphite is formed. The films can be used, for example, as phase plates in a Transmission Electron Microscope.
Abstract:
The invention relates to a method of using a phase plate, having a thin film, in a transmission electron microscope (TEM), comprising: introducing the phase plate in the TEM; preparing the phase plate by irradiating the film with a focused electron beam; introducing a sample in the TEM; and forming an image of the sample using the prepared phase plate, wherein preparing the phase plate involves locally building up a vacuum potential resulting from a change in the electronic structure of the thin film by irradiating the phase plate with a focused beam of electrons, the vacuum potential leading to an absolute phase shift |φ| with a smaller value than at the non-irradiated thin film. Preferably the phase plate is heated to avoid contamination. The phase shift achieved with this phase plate can be tuned by varying the diameter of the irradiated spot.
Abstract:
A freestanding thin film of nano-crystalline graphite is described, as well as a method of producing a freestanding thin film of nano-crystalline graphite including: providing a freestanding thin film of amorphous carbon, heating the freestanding thin film to a high temperature in an inert atmosphere or in a vacuum; and allowing the freestanding thin film to cool down, as a result of which a freestanding thin film of nano-crystalline graphite is formed. The films can be used, for example, as phase plates in a Transmission Electron Microscope.
Abstract:
The invention relates to a method of using a phase plate, having a thin film, in a transmission electron microscope (TEM), comprising: introducing the phase plate in the TEM; preparing the phase plate by irradiating the film with a focused electron beam; introducing a sample in the TEM; and forming an image of the sample using the prepared phase plate, wherein preparing the phase plate involves locally building up a vacuum potential resulting from a change in the electronic structure of the thin film by irradiating the phase plate with a focused beam of electrons, the vacuum potential leading to an absolute phase shift 10 with a smaller value than at the non-irradiated thin film. Preferably the phase plate is heated to avoid contamination. The phase shift achieved with this phase plate can be tuned by varying the diameter of the irradiated spot.
Abstract:
A phase plate, specifically a Zernike type phase plate, for use in an electron microscope, comprises a central hole, and a thin film causing a phase shift of the electrons passing through said film. This phase shift causes the Contrast Transfer Function (CTF) to change from a sine-like function to a cosine-like function.The phase plate is equipped with a film in the form of an annulus, carried by a much thinner film. As a result only in a small spatial frequency range (for low frequencies) the phase is changed (and thus the CTF), and for other spatial frequencies the phase shift is negligible, and thus the CTF remains unchanged. Due to the much smaller thickness of the carrier film the scattering of electrons is negligible as well.