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Fractional topological insulators

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Non-commuting projected position operators<br />

2D: Coordinate transformation<br />

r µ → f µ (r)<br />

<br />

X1 , X 2<br />

<br />

=+i 2 B<br />

<br />

f 1 ( X),f 2 ( X) <br />

=+i 2 B {f 1 ,f 2 } P ( X)+O 4 <br />

B<br />

Poisson bracket<br />

<br />

{f 1 ,f 2 } P<br />

(r) = µν ∂f1 ∂f 2<br />

∂r µ ∂r ν<br />

transformation preserves area<br />

⇒<br />

commutators are unchanged<br />

Thursday, March 22, 2012

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