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Geometry Optimisation with CASTEP

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0.0000000000 0.0000000000 24.5037250000<br />

%ENDBLOCK LATTICE_CART<br />

%BLOCK POSITIONS_FRAC<br />

H 0.2500000000 -0.0103307854 -0.0000000000<br />

H 0.7500000000 -0.0103307854 -0.0000000000<br />

Si 0.5000000000 0.9896692146 0.1662206460<br />

Si 0.5000000000 0.9896692146 0.3878481741<br />

Si 0.2500000000 0.4948346073 0.0554068820<br />

Si 0.2500000000 0.4948346073 0.2770344101<br />

Si 0.7500000000 0.4948346073 0.0554068820<br />

Si 0.7500000000 0.4948346073 0.2770344101<br />

Si 0.0000000000 0.9896692146 0.1662206460<br />

Si 0.0000000000 0.9896692146 0.3878481741<br />

Si -0.0000000000 0.4948346073 0.1108137640<br />

Si -0.0000000000 0.4948346073 0.3324412921<br />

Si 0.7500000000 0.9896692146 0.2216275281<br />

Si 0.5000000000 0.4948346073 0.1108137640<br />

Si 0.5000000000 0.4948346073 0.3324412921<br />

Si 0.2500000000 0.9896692146 0.2216275281<br />

%ENDBLOCK POSITIONS_FRAC<br />

Notice the hydrogen atoms. Now for the constraints on the bottom layer silicon atoms and the hydrogen<br />

atoms (the H atoms must also be constrained because the have a tendency to move into awkward<br />

formations). The list of constraints whose format was specified before looks like<br />

%BLOCK IONIC_CONSTRAINTS<br />

1 H 1 1.00000000 0.00000000 0.00000000<br />

2 H 1 0.00000000 1.00000000 0.00000000<br />

3 H 1 0.00000000 0.00000000 1.00000000<br />

4 H 2 1.00000000 0.00000000 0.00000000<br />

5 H 2 0.00000000 1.00000000 0.00000000<br />

6 H 2 0.00000000 0.00000000 1.00000000<br />

7 Si 3 1.00000000 0.00000000 0.00000000<br />

8 Si 3 0.00000000 1.00000000 0.00000000<br />

9 Si 3 0.00000000 0.00000000 1.00000000<br />

10 Si 5 1.00000000 0.00000000 0.00000000<br />

11 Si 5 0.00000000 1.00000000 0.00000000<br />

12 Si 5 0.00000000 0.00000000 1.00000000<br />

%ENDBLOCK IONIC_CONSTRAINTS<br />

So now we have our supercells ready to run. The calculations were performed on 9 nodes of a Beowulf<br />

cluster. The total final energy per supercell atom as a function of the number of layers of silicon is shown

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