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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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