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Relativistic magnetotransport in graphene, at quantum ... - ICTP

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Dirac fermions <strong>in</strong> <strong>graphene</strong><br />

Honeycomb l<strong>at</strong>tice of C <strong>at</strong>oms<br />

2 massless Dirac cones <strong>in</strong><br />

the Brillou<strong>in</strong> zone:<br />

(Subl<strong>at</strong>tice degree of<br />

freedom ↔ pseudosp<strong>in</strong>)<br />

Fermi velocity (speed of light”)<br />

Close to the two<br />

Fermi po<strong>in</strong>ts K, K’:<br />

Coulomb <strong>in</strong>teractions: F<strong>in</strong>e structure constant<br />

v<br />

F<br />

6 c<br />

≈1.<br />

1⋅10<br />

m s ≈<br />

300<br />

(Semenoff ’84, Haldane ‘88)<br />

Tight b<strong>in</strong>d<strong>in</strong>g dispersion<br />

H<br />

→<br />

≈<br />

p<br />

( p − K)<br />

⋅<br />

r<br />

v p − K<br />

=<br />

r<br />

F<br />

2<br />

e<br />

α ≡<br />

ε hv<br />

F<br />

r<br />

r<br />

σ<br />

vF subl<strong>at</strong>tice<br />

E<br />

= O<br />

( 1)

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