Abstract:
A low energy electron diffraction (LEED) detection module (100) includes: a first vacuum chamber for receiving diffracted electrons from a specimen (109); a larger second vacuum chamber connected to the first vacuum chamber to receive the diffracted electrons that have been transported through the first vacuum chamber; a two-dimensional electron detector disposed in the second vacuum chamber to detect the diffracted electrons; a potential shield (106) disposed generally along an inner surface of the first vacuum chamber and an inner surface of the second vacuum chamber; a magnetic lens (105) to expand a beam of the diffracted electrons that have been transported through the first vacuum chamber towards the two-dimensional electron detector; and a generally plane-shaped energy filter (103) to repel electrons having an energy lower than the probe beam (203) of electrons that impinges on the specimen (109).
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:
New methods for phase contrast imaging in transmission electron microscopy use the imaging electron beam itself to prepare a hole-free thin film for use as an effective phase plate, in some cases eliminating the need for ex-situ fabrication of a hole and reducing requirements for the precision of the ZPP hardware. The electron optical properties of the ZPP hardware are modified primarily in two ways: by boring a hole using the electron beam; and/or by modifying the electro-optical properties by charging induced by the primary beam. Furthermore a method where the sample is focused by a lens downstream from the ZPP hardware is disclosed. A method for transferring a back focal plane of the objective lens to a selected area aperture plane and any plane conjugated with the back focal plane of the objective lens is also provided.
Abstract:
The invention relates to a blocking member to be placed in the diffraction plane of a TEM. It resembles the knife edge used for single sideband imaging, but blocks only electrons deflected over a small angle. As a result the Contrast Transfer Function of the TEM according to this invention will equal that of a single sideband microscope at low frequencies and that of a normal microscope for high frequencies. Preferable the highest frequency blocked by the blocking member is such that a microscope without the blocking member would show a CTF of 0.5.
Abstract:
A method of using a direct electron detector in a TEM, in which an image with a high intensity peak, such as a diffractogram or an EELS spectrum, is imaged on said detector. As known the high intensity peak may damage the detector. To avoid this damage, the centre of the image is moved, as a result of which not one position of the detector is exposed to the high intensity, but the high intensity is smeared over the detector, displacing the high intensity peak before damage results.
Abstract:
A system may include emission of megavoltage radiation from a megavoltage radiation source, acquisition of a first image using an imaging device while first megavoltage radiation is emitted from the megavoltage radiation source and while a plurality of elements is between the megavoltage radiation source and the imaging device, and determination of an amount of scatter radiation based at least on areas of the acquired image corresponding to the plurality of elements. In some aspects, at least one of the plurality of elements is substantially pointed toward a focal spot of the megavoltage radiation source.
Abstract:
An image analysis device 1 is equipped with the photoreceptive means 11 that optically acquires diffraction pattern A that appears on the fluorescent screen 24 in order to obtain the diffraction pattern resulting from reflection high-energy electron diffraction, and the halation-prevention filter 12 provided so as to transmit the visible light emitted from the diffraction pattern A of the fluorescent screen 24, along the light path connecting the photoreceptive means 11 and the fluorescent screen 24. Also, the filter 12 is varied so that the transmittance of the visible light transmitted through the filter 12 is minimum at the filter center and increases with the distance from the center.
Abstract:
In a method for the iterative formation of an image of a specimen in a particle-optical apparatus a series of experimental images (the experimental series) is recorded with each time a different setting of an imaging parameter (for example, the focal distance), and a comparable series of images is calculated on the basis of the electron wave at the specimen (the estimation). The two series are compared and on the basis thereof an electron wave is calculated (the feedback) with which a new series of images is calculated which better approximates the experimental series. This iteration step is repeated until the correspondence between the experimental series and the calculated series is sufficient, after which the associated electron wave is considered to be the desired image of the specimen. A substantial gain as regards calculation time can be achieved during the estimation step as well as during the feedback step by executing the operation of the invention by means of FFTs. This is possible by writing the correlation expressions to be calculated in both steps in accordance with the invention in such a manner that they occur as pure correlation integrals which can be calculated by means of FFTs. The calculation time required when use is made of FFTs is substantially shorter than in the case of explicit calculation of the correlation expressions in conformity with the state of the art. The calculation time can thus be reduced by a factor of the order of magnitude of 50,000.
Abstract:
A system for measuring the thermal characteristic of the surface-lattice of solid state materials with picosecond time resolution uses a picosecond laser pulse which is synchronized with a picosecond electron pulse; the electron pulse being generated by splitting the laser pulse into two beams one of which interacts with the surface under test and the second activates the cathode of an electron gun creating an electron pulse which is, collimated, focused and incident at a small acute angle (1-3 degrees) on the surface. The electron pulse generates a reflection high energy electron diffraction pattern (RHEED) which provides information on the surface temperature in accordance with the Debye-Waller effect. Time resolved measurements are made by using electron pulses which are delayed with respect to the laser pulses by successively greater time intervals.
Abstract:
The invention relates to a system for the deflection of a beam of charged particles, which deflects a particle beam entering at any point into the deflection system such that it impinges upon the entrance orifice of a detector disposed at the exit from the deflection system. The deflection system comprises eight rotationally symmetrically disposed deflection plates and preferably includes two sections in order to achive a large range of uniform field strength in the deflection and a perpendicular impingement of the beam on the detector orifice.