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Ab_init stress perturbation theory - Department of Physics and ...

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DFPT for elastic <strong>and</strong> piezoelectric tensors<br />

• Mixed 2 nd derivatives <strong>of</strong> the energy with respect to two <strong>perturbation</strong>s are<br />

needed.<br />

– By the “2n+1” theorem, these only require one set <strong>of</strong> 1 st order wave functions,<br />

occ<br />

( λλ 1 2) ( λ 2) ( λ1) ( λ1) ( λ1) (0)<br />

el<br />

= ∑ ψα<br />

( +<br />

ext<br />

+<br />

Hxc0)<br />

ψα<br />

α<br />

E T V H<br />

occ<br />

2<br />

+ (0) (0)<br />

∑ ψ + + α<br />

α<br />

2 ∂ ∂ 1 2<br />

• Including atomic relaxation, we need<br />

( λλ 1 2) ( λλ 1 2)<br />

Hxc<br />

( T Vext<br />

) ψα<br />

,<br />

(0)<br />

1<br />

∂ E<br />

λ λ<br />

n<br />

– Clamped-atom elastic tensor ------------<br />

– Internal strain tensor -----------------------<br />

– Interatomic force constants --------------<br />

– Clamped-atom piezoelectric tensor ----<br />

– Born effective charges ---------------------<br />

2<br />

∂ Eel<br />

∂ηαβ∂<br />

2<br />

∂ Eel<br />

∂ηαβ∂<br />

∂<br />

2<br />

2<br />

∂ Eel<br />

∂ηαβ∂<br />

∂<br />

2<br />

E<br />

E<br />

∂! τ′<br />

∂!<br />

τ<br />

el i j<br />

η<br />

! τ<br />

!<br />

γδ<br />

el<br />

∂! τ<br />

i∂E<br />

j !<br />

j<br />

E!<br />

j<br />

Available<br />

Available

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