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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Design <strong>of</strong> development process (continued)<br />
(2)<br />
• Third stage – 0 H 0 :<br />
2<br />
1 ∂ EHxc<br />
E = T + V +<br />
2 ∂ λ ∂ λ<br />
occ<br />
( λ1λ<br />
2) (0) ( λ1λ2)<br />
( λ1λ<br />
2)<br />
(0)<br />
non-var ∑ ψα<br />
(<br />
ext<br />
) ψα<br />
α<br />
– Validate term-by-term with “frozen wave function” numerical strain<br />
derivatives <strong>of</strong> <strong>stress</strong> components<br />
– Diagonal <strong>and</strong> <strong>of</strong>f-diagonal 2DTE’s<br />
1 2<br />
– Numerical strain derivatives <strong>of</strong> forces for internal strain mixed 2DTE’s<br />
– Frozen wf strain derivatives <strong>of</strong> the electric polarization are zero, so there is<br />
no contribution to piezoelectric tensor from these terms<br />
• Note that the numerical derivatives <strong>of</strong> <strong>stress</strong> need factor for<br />
2DTE comparison<br />
2<br />
∂ E el<br />
∂<br />
= Ω<br />
∂η ∂η ∂η<br />
αβ γδ αβ<br />
σ<br />
( σ<br />
γδ )<br />
Ω<br />
n<br />
(0)