Fractional topological insulators
Fractional topological insulators
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 />
∋