Ab_init stress perturbation theory - Department of Physics and ...
Ab_init stress perturbation theory - Department of Physics and ...
Ab_init stress perturbation theory - Department of Physics and ...
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Strain tensor h ab as a <strong>perturbation</strong><br />
• Strain really only changes the positions <strong>of</strong> the atomic (pseudo)potentials,<br />
cell<br />
V () r = V ( r-τ -R) ⎯⎯→ V () r = V [ r-( 1+ η) ⋅τ- ( 1 + η) ⋅R].<br />
ext<br />
∑∑<br />
τ<br />
η ext<br />
R τ R τ<br />
cell<br />
∑∑<br />
• However, this causes unique problems for <strong>perturbation</strong>s expansions:<br />
– Viewed in terms <strong>of</strong> the inf<strong>init</strong>e lattice, the strain <strong>perturbation</strong> can never be<br />
small.<br />
– From the point <strong>of</strong> view <strong>of</strong> a single unit cell, strain changes the periodic<br />
boundary conditions, so wave functions <strong>of</strong> the strained lattice cannot be<br />
exp<strong>and</strong>ed in terms <strong>of</strong> those <strong>of</strong> the unstrained lattice.<br />
• Strain appears to be qualitatively different from other <strong>perturbation</strong>s such<br />
as periodicity-preserving atomic displacements<br />
τ