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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)

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