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Fig. 7 Structural models for WO 6 octahedra in W oxide films made by evaporation onto
substrates at the shown temperatures (RT denotes room temperature). Arrows in the x and
y directions are 2 nm long. After Nanba and Yasui ( 1989 )
Fig. 8 Schematic diagram
showing thin-film
nanostructures for different
pressures in the sputter
plasma and for different
substrate temperatures. The
material's melting
temperature is denoted s m .
From Thornton ( 1974 )
is desirable for electrochromic applications. It is of interest to notice in this context
that the deposition may involve molecular species, and trimeric W 3 O 9 molecules
are well known to form during evaporation (Maleknia et al. 1991 ), while a pre-
ponderance of (W 6 O 19 ) 2- (known as ''Lindqvist anions'') may be present in
aqueous solutions (Lang et al. 2012 ) used for liquid-phase thin-film deposition.
2.3 Optical Absorption Mechanisms
The reason for the variable optical absorption in electrochromic materials has been
discussed extensively and is a complicated issue for several reasons. First of all, the
oxides are often poorly defined regarding crystallinity, and they can incorporate
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