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146nm 2 obtained from Fig. 2). 1. Adsorption and Desorption 55 For a better understanding and in order to avoid fundamental errors it is necessary to check the thickness dependence of the absolute resistivity change. The existing models concerning the classical size effect predict a proportionality to d -1 as a first approach. Such a dependence has been seen for example, for CO adsorbed on Ni films by WiBmann (Wit~mann 1975) and for gold on gold films at low temperatures by Fischer (Fischer 1980).
Only the pure gold films show a striking structural difference. The terrace edges of these 48 4. Thin Metal Films on Glass Supports films consist of rather straight parts which always create angles of 120 ~ or 60 ~ to each other. 4 E l e c t r i c a l C o n d u c t i v i t y The measurement of the electrical conductivity has already been used to find the optimum evaporation conditions as described in the first part of this chapter. Here the electrical properties of the films are described independently of the controversial thin film conductivity models as much as possible.
2 [For details see: Persson (1991)]. 146nm 2 obtained from Fig. 2). 1. Adsorption and Desorption 55 For a better understanding and in order to avoid fundamental errors it is necessary to check the thickness dependence of the absolute resistivity change. The existing models concerning the classical size effect predict a proportionality to d -1 as a first approach. Such a dependence has been seen for example, for CO adsorbed on Ni films by WiBmann (Wit~mann 1975) and for gold on gold films at low temperatures by Fischer (Fischer 1980).