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

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Boltzmann approach<br />

Boltzmann equ<strong>at</strong>ion <strong>in</strong> Born approxim<strong>at</strong>ion<br />

⎛<br />

⎜<br />

⎝<br />

a.) +, i +, i<br />

−, i<br />

∂ ⎞<br />

+ eE⋅<br />

⎟ f<br />

∂k<br />

⎠<br />

Cb<br />

2<br />

( k,<br />

t)<br />

= I [ k,<br />

t | { f ( k′<br />

, t)<br />

} ] ∝ α ( T )<br />

∂ t<br />

±<br />

coll<br />

±<br />

b.)<br />

−, i<br />

1<br />

2<br />

−<br />

+, i +, i<br />

−, i<br />

+, i +, i<br />

+, i<br />

+, i<br />

−, i<br />

−<br />

2<br />

L. Fritz, J. Schmalian, MM, and S. Sachdev, PRB 2008<br />

+(N − 1)<br />

+, i +, i<br />

−, j<br />

−, j<br />

2<br />

+(N − 1)<br />

+, i +, i +, i +, i<br />

2<br />

+, i<br />

Collision-limited conductivity:<br />

+, i<br />

+(N − 1)<br />

+, j<br />

0.<br />

76<br />

σ ( μ = 0)<br />

= 2<br />

α<br />

+, j<br />

e<br />

2<br />

( T ) h<br />

+, i +, j<br />

−, j<br />

2<br />

−, i<br />

2

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