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Table A.2

Binding energies for (TiO2)n clusters.

Molecule D0(n) [eV] D0(n) /n [eV] ΔE(n) [eV] D0(n)/(x + y) [eV]

TiO2 12.42 12.42 12.42 4.14
(TiO2)2 30.24 15.12 18.00 5.04
(TiO2)3 47.59 15.86 17.35 5.29
(TiO2)3Bromley 48.10 16.03 17.86 5.34
(TiO2)4 65.05 16.26 17.46 5.42
(TiO2)4Bromley 66.28 16.57 18.18 5.52
(TiO2)5 82.46 16.49 17.41 5.50
(TiO2)5Bromley 84.30 16.86 18.02 5.62
(TiO2)6 99.88 16.65 17.42 5.55
(TiO2)6Bromley 103.30 17.22 19.00 5.74
(TiO2)7Bromley 121.48 17.35 18.18 5.78
(TiO2)8Bromley 139.89 17.49 18.41 5.83
(TiO2)9Bromley 158.14 17.57 18.25 5.86
(TiO2)10Bromley 176.86 17.69 18.72 5.90

Notes. Total binding energy D0(n), binding per monomer D0(n) /n, energy gain ΔE(n) by adding a monomer, and the binding energy per atom D0(n)/(x + y). Bromley energies have larger binding energies that the original Jeong geometries.

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