Abstract:
In a transmission electron microscope with phase contrast imaging, the illumination of the object to be imaged takes place with an annular illuminating aperture. An annular phase-shifting element with a central aperture is arranged in a plane Fourier transformed with respect to the object plane. The annular phase-shifting element confers a phase shift of &pgr;/2 on a null beam, while the radiation of higher diffraction orders diffracted at the object in the direction of the optical axis passes through the central aperture of the annular phase-shifting element and consequently is not affected, or only slightly affected, by the phase-shifting element. The annular illuminating aperture is preferably produced sequentially in time by a deflecting system, which produces a beam tilt in a plane conjugate to the object plane.
Abstract:
An energy filter, particularly for electron microscopes, in which the setting of different energy bandwidths takes place electron-optically. For this purpose, one or more deflecting systems and one or more transfer lenses are provided at the filter exit. A diaphragm arrangement is arranged in the dispersion plane and has an opening with a stepped edge region. Slit diaphragms with different slit lengths can be simulated by deflection of the electron beam. The deflection of the electron beam effected by the dispersion system(s) perpendicularly to the dispersive direction of the filter is compensated again by a succeeding transfer lens or a further deflecting system, so that an image displacement is also compensated. In a second embodiment, a respective slit edge is arranged in two mutually conjugate spectrum planes. A deflecting system preceding each slit edge, different spectrum portions are filtered out by the two slit edges, according to the excitation of the deflecting systems. The energy bandwidth can be varied continuously in this embodiment.
Abstract:
The invention is directed to a method of illuminating an object in a transmission electron microscope. For illuminating the object, two condenser lenses are used such that they image an image of the electron source with different demagnifications. This crossover is imaged in the focal plane of a single-field condenser objective lens by means of a third condenser lens 14 for TEM-operation whereby the illumination aperture can be adjusted with respect to its magnitude. The electron beam is shaped ahead of the single-field condenser objective lens by two diaphragms arranged in different planes and by means of at least one deflection system such that the magnitude of the illumination field on the object is only slightly larger than the region magnified by the electron microscope. The magnitude of the illumination field and the illuminating aperture can be adjusted independently of each other.