![](/images/gifchars/beta2.gif)
-[SiW
12O
40]
4- (
C3v symmetry) is sufficiently higher in energy thanits
![](/images/gifchars/alpha.gif)
-isomer analogue that effectively complete conversion to
![](/images/gifchars/alpha.gif)
-[SiW
12O
40]
4- (
Td) is observed. By contrast,
![](/images/gifchars/beta2.gif)
- and
![](/images/gifchars/alpha.gif)
-[AlW
12O
40]
5-(
![](/images/gifchars/beta2.gif)
- and
![](/images/gifchars/alpha.gif)
-
1;
C3v and
Td, respectively) are sufficiently close inenergy that both isomers are readily seen in
27Al NMR spectra ofequilibrated (
![](/images/gifchars/alpha.gif)
-
![](/images/gifchars/beta2.gif)
) mixtures. Recently published DFT calculationsascribe the stability of
![](/images/gifchars/beta2.gif)
-
1 to an electronic effect of the large,electron-donating [AlO
4]
5- (
Td) moiety encapsulated within thepolarizable, fixed-diameter
![](/images/gifchars/beta2.gif)
-W
12O
36 (
C3v) shell. Hence, no uniquestructural distortion of
![](/images/gifchars/beta2.gif)
-
1 is needed or invoked to explain itsunprecedented stability. The results of these DFT calculations areconfirmed by detailed comparison of the X-ray crystal structure of
![](/images/gifchars/beta2.gif)
-
1 (
![](/images/gifchars/beta2.gif)
-Cs
4.5K
0.5[Al
IIIW
12O
40]·7.5H
2O; orthorhombic, space group
Pmc2
1,
a = 16.0441(10) Å,
b = 13.2270(8) Å,
c = 20.5919(13)Å,
Z = 4 (
T = 100(2) K)) with previously reported structures of
![](/images/gifchars/alpha.gif)
-
1,
![](/images/gifchars/alpha.gif)
- and
![](/images/gifchars/beta2.gif)
-[SiW
12O
40]
4-, and
1-[SiMoW
11O
40]
4-.