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My PhD thesis - Condensed Matter Theory - Imperial College London

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LIST OF FIGURES<br />

5.3 The LDA energy per electron as a function of the number of grid<br />

points. Cells of size w ∼105 and w ∼210 are compared, both for<br />

finite systems containing 360 electrons and for systems infinite in the<br />

xy-direction. Note that the two vertical scales are offset. The slab<br />

width is 17.64248; the density parameter is r s = 2.07. The length of<br />

the cell in the z-direction varies slightly as a function of the number<br />

of grid points; this is to ensure optimal sampling of the important<br />

slab region. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 77<br />

5.4 The dependence of the LDA energy per electron on the slab width;<br />

for this system, r s = 2.07, the number of electrons is 360 and the cell<br />

size in the z-direction is around 105. . . . . . . . . . . . . . . . . . . 78<br />

5.5 The surface energy as a function of slab width, calculated using different<br />

values of the bulk energy. The middle curve uses the Perdew-<br />

Wang parameterisation [69] of Ceperley and Alder’s early QMC results<br />

[12], which was the functional employed in the slab calculation.<br />

The upper curve is from the Perdew-Zunger [70] paremeterisation of<br />

the same results; the lower curve is from the Perdew-Zunger parameterisation<br />

of Ortiz and Ballone’s later QMC calculations [63]. . . . . 79<br />

5.6 The components of the LDA surface energy as a function of the slab<br />

width. All the surface energies are given in mHa bohr −2 . . . . . . . . 80<br />

5.7 The distribution of configuration energies, before and after variance<br />

minimisation. 10000 configurations have been included; the Jastrow<br />

factor was of the form introduced in section 3.4.1 and described in<br />

detail in section 6.3. Optimisation of both u and χ terms was allowed;<br />

The minimisation was performed without reweighting. . . . . . . . . . 81<br />

6.1 The total VMC energy per electron as a function of system size,<br />

comparing the Ewald and MPC interactions. The exchange energy<br />

given by equation (6.25) is also plotted (note the different vertical<br />

scale). Energies, as usual, are in Ha. . . . . . . . . . . . . . . . . . . 90<br />

9

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