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Quasiparticle interference in the pseudogap phase of cuprate ...

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QP INTERFERENCE 12<br />

Nodal approximation: importance <strong>of</strong> coherence factors<br />

One f<strong>in</strong>ds<br />

Λ(q, iω) = 1 L 2 ∑<br />

k<br />

(iω + ɛ + )(iω + ɛ − ) − ∆ + ∆ −<br />

(ω 2 + E+)(ω 2 2 + E−)<br />

2 ,<br />

k<br />

y<br />

with ɛ ± = ɛ<br />

√ k±q/2 , ∆ ± = ∆ k±q/2<br />

and E ± = ɛ 2 ± + ∆ 2 ±. L<strong>in</strong>earize<br />

near <strong>the</strong> nodes to obta<strong>in</strong><br />

v<br />

−<br />

F<br />

v∆<br />

Q’<br />

Q<br />

+<br />

v<br />

∆<br />

v<br />

F<br />

−<br />

k 2 k 1<br />

k<br />

x<br />

v<br />

F<br />

v<br />

∆<br />

+<br />

v<br />

∆<br />

v<br />

F<br />

Λ l<strong>in</strong> = 1<br />

v F v ∆<br />

∫<br />

d 2 k<br />

(2π) 2 −ω 2 + (k 2 1 − k 2 2) − (˜q 2 1 − ˜q 2 2)<br />

[ω 2 + (k + ˜q) 2 ][ω 2 + (k − ˜q) 2 ] .<br />

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