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Quasiparticle interference in the pseudogap phase of cuprate ...

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QP INTERFERENCE 16<br />

This <strong>the</strong>ory describes fermionic<br />

excitations <strong>in</strong> a <strong>phase</strong>-disordered<br />

d-wave superconductor. The electron<br />

propagator reads<br />

QED 3<br />

[Franz and Tešanović, PRL 87, 257003 (2001)]<br />

G 0 (k, iω) = λ −η iω + ɛ k σ 3<br />

[ω 2 + ɛ 2 k + ∆2 k ]1−η/2,<br />

where λ is a high energy cut<strong>of</strong>f<br />

and η is <strong>the</strong> anomalous dimension<br />

exponent which encodes <strong>the</strong> physics<br />

<strong>of</strong> <strong>phase</strong> fluctuations. η is a small<br />

positive number, whose precise value<br />

is still under debate.<br />

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