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Topological Insulators - GDR Meso

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Anisotropic Scattering of Dirac states<br />

Consider Dirac surface states with<br />

‣ phase coherence (small sample, low T)<br />

‣ scalar disorder<br />

‣ semi-classical limit<br />

H 0 = ~v F ẑ ⇥ (~ ⇥ ~ k)<br />

+V (~r )<br />

(high doping in the gap)<br />

Hexagonal warping :<br />

L. Fu, PRL 103 (2009)<br />

H W = z 2<br />

k+ 3 + k 3 k ± = k x ± ik y<br />

b w = E2 F<br />

‣ allowed by Time Reversal Symmetry (same univ. class)<br />

‣ experimentally extracted value in TI : bw=0.4-0.6<br />

‣ important at high kF (weak localization regime)<br />

‣ Perturbative parameter (deformation of Fermi surface) bw<br />

➡ depends on EF<br />

Anisotropic scattering :<br />

‣ comes from pure (Dirac) Hamiltonian, not disorder<br />

‣ strongly increased by warping term<br />

k min<br />

2~ 3 v 3 F<br />

kmax<br />

Scattering amplitude<br />

bw=0.6 bw=0.0<br />

f(✓, ✓ 0 ✓)=|h ~ k|V | ~ k 0 i|<br />

✓ =0 ✓ = ⇡/6<br />

mardi 3 janvier 12

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