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1
2
S 10
C i
3
C 1
Figure 33. Three of the 30026 H-bond isomers of the (H 2 O) 20 dodecahedron [25]. Structure (1)
is a high-symmetry ( S 10 ), and also high-energy structure. Structure (2) is of C i symmetry, and structure
(3), a very stable structure, has no symmetry ( C 1 ).
Graph invariants, constructed using the point group operations of a finite cluster,
provide a precise way to link scalar physical properties of clusters to their H-bond
topology.
C r
α
I r =
g α ( b r )
(44)
C rs
α
I rs =
g α ( b r b s )
(45)
C rst
α
I rst =
g α ( b r b s b t )
(46)
···
In the above equations, the sums are over all elements g α of the cluster point group,
and Eqs. (44)-(46) generate first-, second-, and third-order invariants, respectively,
for finite water clusters. In line with our experience for ice, we have never found
the need to go further than second-order invariants to describe water clusters.
The (H 2 O) 20 dodecahedron provides an example of the ability of graph invari-
ants to organize and describe scalar physical properties among H-bond isomers.
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