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Topological Insulators - GDR Meso

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(Weak) Localization<br />

• Probability to diffuse from ⇥r to ⇥r<br />

⇥<br />

P (⌅r ⌅r ⇥ ) ⇥<br />

path C ⇥r<br />

• Phase variation along a diffusion path :<br />

• Average interferences vanish,<br />

except if ”C = C ” (reversed ring)<br />

⇥r ⇥<br />

A C<br />

2<br />

= ⇥ |A C | 2 + ⇥ A C A C ⇥<br />

C<br />

C⇤=C ⇥<br />

⌅ C =2⇤ L C<br />

⇥ F<br />

Classical<br />

Interferences<br />

random in a metal<br />

B<br />

• Phase coherent corrections<br />

‣ loop contributions<br />

O ⇤ C,C =2⇥ C,C / 0<br />

➡Effective diffusion of «pseudo particles» Diffuson (same dir.) / Cooperon (opp. dir.)<br />

0.2<br />

0<br />

-0.2<br />

-0.4<br />

-0.6<br />

-0.8<br />

2.10 - 5 690 mK<br />

11.2<br />

11<br />

10.8<br />

0 20 40 60 80 100<br />

-2000 0 2000<br />

Conductance, same sample, different spins config.<br />

12.4<br />

12.2<br />

12<br />

11.8<br />

11.6<br />

11.4<br />

Flux Through the Sample<br />

mardi 3 janvier 12

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