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Additional resources for IBM 31P2-2FSQ7-112 Theory of Programming for AN FSQ-7 Combat Direction Central
S. tend to have a behaviour similar to the bulk one. S. on surfaces exist for all the transition metals and have been observed by spectroscopy. e. high index surfaces) were reported, particularly in the case of pt 9 • This suggests that electronic properties may differ markedly from surface site to surface site in heteregeneous surface. S. S. at the protruding edge of the stepped surfaces of Pt and the symmetry of states near the Fermi level is found to be rather dependent on the geometry of the surface lO (Fig.
18. : 1969, Int. J. Quant. Chern. 3 S, p. 179. 19. : 1972, J. Chern. Phys. 57, p. 4870. 20. : 1978, Theoret. Chirn. Acta 49, p. 143. 21. : 1964, Phys. Rev. 136 B, p. 864. 22. : 1965, Phys. Rev. 140 A, p. 1133. 23. : 1976, Phys. Rev. B'13, p. 4274. 24. 211. 25. : 1979, J. Am. Chern. Soc. 101, p. 3821. 26. : 1980, Faraday Symp. 14, p. 170. 27. : 1979, Inorg. Chern. 18, p. 2782. CHEMISORPTIVE PROPERTIES OF TRANSITION METAL CLUSTERS F. S. P. 166, 38042 Grenoble Ced8x, Franc8 Ch8misorptiv8 properties of simple gas8s on transition metal clust8rs ar8 shown to be closely r8lated to their 8lectronic properties.
And give information on the spatial distribution of electrons in the vafious orbitals A. 1 Semi-infinite transition metal surfaces One can resume the detailed results obtained for various cleavage pleanes and various crystallographic structures in the following way6 - For a dense cleavage plane (Le. S. 2a). - For a non dense cleavage plane such as the (110) for a FCC lattice or the (100) for a BCC lattice, it exists a virtual bound state peak in the middle of the band. S. at the top of the band (Fig.