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Fig. 6 Structures
representing W oxide with
the shown structures. Dots
indicate sites for ion insertion
in open spaces between WO 6
octahedra. Dashed lines
signify extents of the unit
cells. From Granqvist ( 1995 )
spaces between the octahedral units are larger than for the cubic structure, as
indicated in Fig. 6 b. Hexagonal structures, which are delineated in Fig. 6 c, seem
to be formed easily in thin films (Granqvist 1995 ), and then, the structure is even
better for ion transport.
The actual nanostructures in thin films of W oxide have been studied several
times, and Fig. 7 reports data based on modeling of X-ray scattering from samples
made by evaporation onto substrates at different temperatures (Nanba and Yasui
1989 ). A cluster-type structure is apparent with hexagonal-like units that grow and
interconnect at sufficiently high substrate temperatures.
The relationship between nanostructure and thin-film deposition parameters can
often be well illustrated through ''zone diagrams,'' which have been reported for
different deposition techniques and with different degrees of detail. Figure 8 shows
a ''Thornton diagram'' for the particular case of sputter deposition (Thornton
1974 ); more elaborate versions can be found elsewhere (Barna and Adamik 1998 ;
Anders 2010 ). It is evident that low substrate temperatures and high pressures in
the discharge plasma for the sputtering lead to nanoporous structures of a kind that
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