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arxiv: 1104.0364 · v2 · pith:OBPU2OOXnew · submitted 2011-04-03 · ❄️ cond-mat.supr-con · cond-mat.str-el

Reaffirming the d_(x²-y²) superconducting gap using the auto-correlation angle-resolved photoemission spectroscopy of Bi_(1.5)Pb_(0.55)Sr_(1.6)La_(0.4)CuO_(6+δ)

classification ❄️ cond-mat.supr-con cond-mat.str-el
keywords arpesspectroscopyangle-resolvedaroundcanonicalft-stsmathrmmodel
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Knowledge of the gap function is important to understand the pairing mechanism for high-temperature ($T_\mathrm{c}$) superconductivity. However, Fourier transform scanning tunneling spectroscopy (FT STS) and angle-resolved photoemission spectroscopy (ARPES) in the cuprates have reported contradictory gap functions, with FT-STS results deviating strongly from a canonical $d_{x^2-y^2}$ form. By applying an "octet model" analysis to autocorrelation ARPES, we reveal that a contradiction occurs because the octet model does not consider the effects of matrix elements and the pseudogap. This reaffirms the canonical $d_{x^2-y^2}$ superconducting gap around the node, which can be directly determined from ARPES. Further, our study suggests that the FT-STS reported fluctuating superconductivity around the node at far above $T_\mathrm{c}$ is not necessary to explain the existence of the quasiparticle interference

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