Observations on small vapour-deposited particles of silver and gold with direct lattice imaging in the Cambridge University 600 kV high-resolution electron microscope have established unambiguously the presence of dislocations in particles as small as 15nm in diameter. The detailed structure of more complicated ' polyparticles ' can also be characterized directly. Knowledge of the internal and surface structure of small metallic particles is basic to an understanding of the nucleation of thin metal films and any explanation of their important role in heterogeneous cataIysis. Observations using electron diffraction and electron microscopy have proved invaluable in elucidating their crystallography, in particular in establishing the existence of multiple twinning within many particles (In0 1966, Ino and Ogawa 1967, Allpress and Sanders 1967). These so-called multiple-twinned particles (MTPs) are known to be composed of either five or twenty tetrahedra which make up decahedra or icosahedra. (The icosahedral MTPs have a similar topological structure to spherical viruses (Caspar and Klug 1961) and geodesic domes (Fuller 1963).) However, such arrangements of tetrahedra are not completely space-filling, and some form of Iattice distortion or imperfection is required. Lattice imaging with axial illumination at 100 kV has been used previously to observe evaporated gold particles (Komoda 1968). Typically however, with an objective lens defocus, AZ, appropriate for best visibility of (111) lattice fringes of about 0.2-0-4 pm (given by A2 = Cs81112, where C, is the spherical aberration coefficient of the objective lens and 0111 is the diffraction angle), information about lattices of other periodicities cannot be seen unless the coherence of the incident illumination is adequate, and it is then considerably misplaced. At operating voltages of 500 kV or more the diffraction angles are much smaller than at 100 kV, substantially reducing the fringe displacements. Furthermore, the increased spatial coherence of the illumination afforded by the high-brightness lanthanum hexaboride electron gun
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