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Itinerant Spin Dynamics in Structures of ... - Jacobs University

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136 Appendix B: L<strong>in</strong>ear Response<br />

Furthermore we assume low temperature which is why the derivative <strong>of</strong> the Fermi<br />

function fixes the energy <strong>of</strong> the Green’s functions to the Fermi energy,<br />

− ∂f T=0<br />

∂E = δ(E −E F).<br />

(B.34)<br />

We end up with<br />

σ impx,x (0) = 1<br />

πV<br />

e 2<br />

m 2 e<br />

∑<br />

k x k ′ 〈<br />

x G<br />

R<br />

E (k,k ′ )G A E (k′ ,k) 〉 . (B.35)<br />

imp<br />

k,k ′

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