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Table 1:
Average binding energy per electron
for carbon and boron nitride systems. The energies of the
graphitic phases are for isolated sheets.
|
|
|
|
C systems |
|
|
BN systems |
Benzene |
2.24 |
1.99 |
Borazine |
PPV |
2.22 |
1.98 |
PVB |
PPP |
2.22 |
1.98 |
PBZ |
Graphite |
2.20 |
1.96 |
Graphitic BN |
To investigate the energetics of these different structures, we have
calculated their total binding energies with respect to their
constituent atoms.
Trends in the energetics can be observed in both the average bond
energies (i.e. the total binding energy divided by the number of
bonds in the structure) [27] and the
binding energy per electron
(i.e. the total binding energy divided by the number
of valence electrons), which we report in
Table 1.
We compare the energies of the (one-dimensional)
polymers to the (zero-dimensional) molecules (benzene and borazine)
used to build them, and to the corresponding (two-dimensional) graphitic forms.
As expected, the polymers fall energetically in between these two extremes,
with the same trend for the boron nitride and the carbon compounds,
and small energy variations within compounds of the same family.
This suggests that the chemistry of the BN polymers should be similar to
that of the carbon polymers.
Next: Band structures and wavefunctions
Up: Material design from first
Previous: Structures
Peter D. Haynes
2002-10-28