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Reaffirming the
d
x
2
−
y
2
d_{x^2-y^2}
d
x
2
−
y
2
superconducting gap using the auto-correlation angle-resolved photoemission spectroscopy of Bi
1.5
_{1.5}
1.5
Pb
0.55
_{0.55}
0.55
Sr
1.6
_{1.6}
1.6
La
0.4
_{0.4}
0.4
CuO
6
+
δ
_{6+\delta}
6
+
δ
Authors
T. P. Devereaux
H. Eisaki
+9 more
M. Hashimoto
R. -H. He
Z. Hussain
D. H. Lu
W. Meevasana
R. G. Moore
Z. -X. Shen
J. P. Testaud
Y. Yoshida
Publication date
22 April 2011
Publisher
'American Physical Society (APS)'
Doi
View
on
arXiv
Abstract
Knowledge of the gap function is important to understand the pairing mechanism for high-temperature (
T
c
T_\mathrm{c}
T
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
d_{x^2-y^2}
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
d_{x^2-y^2}
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
c
T_\mathrm{c}
T
c
is not necessary to explain the existence of the quasiparticle interferenceComment: 5 page
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Last time updated on 22/04/2021