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 />
• Fourth stage –<br />
2<br />
– Use strain-<strong>perturbation</strong> wave functions<br />
– is Cartesian strain or reduced atomic displacement<br />
λ 1<br />
• Electric field is special case –<br />
occ<br />
( λ 1 λ 2) ( 2) ( 1) ( 1) ( 1) (0)<br />
non-stat<br />
= ∑ ψ<br />
λ ( λ λ λ<br />
α<br />
+<br />
ext<br />
+<br />
Hxc0)<br />
ψα<br />
α<br />
( λ )<br />
ψ α<br />
E T V H<br />
∂ E 2Ω<br />
∑<br />
∂E ! !<br />
∂<br />
2 occ<br />
( k!<br />
el<br />
j ) ( η )<br />
=<br />
iψ<br />
3<br />
m<br />
ψ<br />
αβ<br />
m<br />
d<br />
j<br />
ηαβ<br />
(2 π )<br />
∫ k k<br />
k<br />
BZ m<br />
– Field <strong>and</strong> d/dk first-order wave function in reduced coordinates<br />
Non-selfconsistent<br />
• Validate using numerical strain derivatives <strong>of</strong> GS <strong>stress</strong>es, forces, <strong>and</strong><br />
polarization<br />
– Use converged strained wave functions<br />
– No subtractions since non-variational contributions are already validated<br />
– For polarization, numerical derivatives have to be corrected to give “proper”<br />
piezoelectric tensor (see Infos/<strong>theory</strong>/lr.pdf)<br />
– Need to use f<strong>init</strong>e-difference d/dk wf’s in RF calculation for accurate<br />
comparison