Quasiparticle interference in the pseudogap phase of cuprate ...
Quasiparticle interference in the pseudogap phase of cuprate ...
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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