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Fractional topological insulators

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= 0<br />

γ x<br />

3-fold<br />

9-fold<br />

0 10 20<br />

Topological insulator: 2/3 0filling<br />

1 2 3 U/V<br />

c) a)<br />

d)<br />

U/V = 0, λ = 1 U/V = 3, λ = 1<br />

1<br />

λ<br />

0.5<br />

2ϖ<br />

γ x<br />

!<br />

%<br />

$./<br />

!"<br />

3-fold<br />

9-fold<br />

0 ϖ 2ϖ 0 ϖ γ 2ϖ<br />

x<br />

'()*+,<br />

-()*+,<br />

0<br />

0 1 2 3 U/V<br />

b)<br />

c)<br />

E/V<br />

0.2<br />

0.1<br />

0<br />

U/V = 0, λ = 0<br />

0 ϖ<br />

γ x<br />

Thursday, March 22, 2012<br />

2ϖ<br />

U/V = 0, λ = 1<br />

d)<br />

U/V = 3, λ = 1<br />

$ %$ &$<br />

B 0,k := 0,<br />

$<br />

$ % & ' !"#<br />

B 1,k +iB 2,<br />

#"<br />

2" ,"<br />

!"#()($01!"#"$ !"#()($01!"#"% !"#()('01!"#"%<br />

B 3,k := 2t<br />

H 2<br />

int := U ρ i,↑ ρ i,↓ + V<br />

<br />

ρi,↑ ρ j,↑ + ρ i,↓ ρ j,↓ +2λρ i,↑ ρ j,↓<br />

i∈Λ<br />

ij∈Λ<br />

and the three Pau<br />

sublattice index.<br />

γ x<br />

2ϖ 0 ϖ<br />

neighbor (NN) an<br />

ping amplitudes.<br />

$"#<br />

$.&<br />

$.%<br />

∋<br />

0 10 20<br />

E/V<br />

0 ϖ γ x<br />

2ϖ<br />

∋<br />

0.2<br />

0.1<br />

0<br />

3-fold<br />

9-fold<br />

0 10 20<br />

0 1 2 3 U/V<br />

b)<br />

c)<br />

U/V = 0, λ = 0<br />

0 ϖ<br />

γ x<br />

2ϖ<br />

d)<br />

U/V = 0, λ = 1 U/V = 3, λ = 1<br />

&<br />

lattice momentum<br />

α = A, B and c<br />

ψ † k,σ := c † k,A,σ ,<br />

single-particle Ha<br />

H 0 := <br />

0 ϖ γ 2ϖ 0 ϖ<br />

x<br />

γ 2ϖ<br />

x<br />

k∈BZ<br />

ψ † k<br />

where the 3-vecto<br />

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