QuantumATK Forum
QuantumATK => General Questions and Answers => Topic started by: Weckman on November 24, 2021, 22:20
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I would like to study the stability of different surface orientations of wurtzite/zinc blende materials which exhibit asymmetric surfaces for certain lattice orientations and therefore would like to use the periodic surface model (electrode) to compute the relative stabilities of these surfaces.
I do not yet have the full licence in my disposal, so I ran some test calculations on my desktop for Au(111) surface. However, when I compute the total energy of surfaces with varying thickness, in some instances I get negative surface energies.
For example, when using surfaces with 6 and 8 layers of gold, medium basis set and SG15 pseudo, I get energies
6 -22519.98379
7 -26273.25555
8 -30026.51107
Making a linear fit gives a slope of -3751.264 eV, close to that of a bulk calculation (-3753.231 eV). However, the intercept is negative and so is the surface energy.
If I use a HGH pseudo, I get a positive surface energies that vary depending on the basis set used.
What I would like to know:
Is this a correct approach to take and are the results some kind of an artifact resulting from a thin surface model or am I making a fundamental error somewhere or how should I approach the issue? In the original paper ("First-principles Green’s-function method for surface calculations: A pseudopotential localized basis set approach") the authors discuss developing the procedure for SG15 pseudos. However, QuantumATK allows me to set from a variety of different pseudos. Is the Green's function method suitable for all the available pseudos and basis sets?
- Weckman
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This presentation is relatively clear about how to compute the surface energy: https://sites.psu.edu/dftap/2019/03/25/evaluating-surface-energy-calculations-of-pt111-for-different-slab-model-parameters/