My PhD thesis - Condensed Matter Theory - Imperial College London
My PhD thesis - Condensed Matter Theory - Imperial College London
My PhD thesis - Condensed Matter Theory - Imperial College London
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CHAPTER 5.<br />
THE JELLIUM SLAB<br />
Here ∆ɛ slab is the error in the calculated energy per electron of the slab and ∆σ is<br />
the resultant error in the jellium surface energy. Equation (5.1) has been used to<br />
relate the number of electrons per unit area N/A to the density parameter r s . For a<br />
slab width of 20.0, setting ∆σ = 50 erg cm −2 gives ∆ɛ slab ≈ 0.1 mHa (or 3 meV) per<br />
electron. This gives an idea of the accuracy needed in the Monte Carlo simulations.<br />
5.3 Preliminary investigations<br />
The surface energy of jellium is defined in the limit of an infinitely-wide slab with<br />
infinite extent in the xy-direction. In DFT, it is possible to achieve one of these<br />
limits. Because the external (background) potential does not depend on x or y, the<br />
system is homogeneous in the xy-plane; the non-interacting Kohn-Sham orbitals<br />
have the simple form<br />
φ nk‖ (r) = u n (z)e ik ‖·r ‖<br />
. (5.5)<br />
The density of states in k ‖ -space is therefore constant, and extrapolation to a system<br />
with infinite xy-extent is trivial. This is how the infinite-system density profiles<br />
displayed in figures 5.1 and 5.2 were obtained.<br />
Unfortunately, this simple extrapolation is not possible in QMC simulations,<br />
which must use a finite number of electrons; for this reason, it is useful to study<br />
finite cells in DFT.<br />
The DFT simulations are carried out on a grid in the z-direction which extends<br />
for some distance outside the slab, using a code supplied by Pablo Garcia-Gonzalez<br />
[26]. It is important to ensure that the results are converged with respect to both<br />
the number of grid points used and the spacing of these points (or equivalently, the<br />
effective cell size in the z-direction, which will be denoted as w).<br />
Figure 5.3 shows the results of convergence testing, for both the finite and infinite<br />
horizontal cells. Cells of two different lengths in the z-direction have been compared:<br />
even the smaller of these is around five times larger than the slab width, and the<br />
figure demonstrates that in this regime the cell size is unimportant. What matters is<br />
the sampling of the slab region: this is why the results for a cell size of 105 with 512<br />
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