2013
DOI: 10.1073/pnas.1302932110
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Universal features in the photoemission spectroscopy of high-temperature superconductors

Abstract: The energy gap for electronic excitations is one of the most important characteristics of the superconducting state, as it directly reflects the pairing of electrons. In the copper-oxide hightemperature superconductors (HTSCs), a strongly anisotropic energy gap, which vanishes along high-symmetry directions, is a clear manifestation of the d-wave symmetry of the pairing. There is, however, a dramatic change in the form of the gap anisotropy with reduced carrier concentration (underdoping). Although the vanishi… Show more

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Cited by 15 publications
(13 citation statements)
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“…While the near-nodal gap appears to be approximately x independent for a broad range of doping below optimal (Vishik et al, 2012;da Silva Neto et al, 2013), the antinodal gap increases with decreasing x. Sharp "quasiparticle" peaks with energy ΔðkÞ and width small compared to the antinodal gap energy exist along the entire Fermi surface, again with the possible exception of highly underdoped samples (Vishik et al, 2012;Zhao et al, 2013). Likewise, in single-layer ðBi; PbÞ 2 ðSr; LaÞ 2 CuO 6þδ , quasiparticle peaks are harder to identify, but by looking at the difference between the spectra above and below T c , coherent quasi-particle-like features have been identified around the entire Fermi surface, but only for doping above optimal (Kondo et al, 2009).…”
Section: A Spectroscopic Characterizationsmentioning
confidence: 93%
“…While the near-nodal gap appears to be approximately x independent for a broad range of doping below optimal (Vishik et al, 2012;da Silva Neto et al, 2013), the antinodal gap increases with decreasing x. Sharp "quasiparticle" peaks with energy ΔðkÞ and width small compared to the antinodal gap energy exist along the entire Fermi surface, again with the possible exception of highly underdoped samples (Vishik et al, 2012;Zhao et al, 2013). Likewise, in single-layer ðBi; PbÞ 2 ðSr; LaÞ 2 CuO 6þδ , quasiparticle peaks are harder to identify, but by looking at the difference between the spectra above and below T c , coherent quasi-particle-like features have been identified around the entire Fermi surface, but only for doping above optimal (Kondo et al, 2009).…”
Section: A Spectroscopic Characterizationsmentioning
confidence: 93%
“…The first one may be related to superconductivity and appears at the superconducting transition temperature, where the resistance vanishes. The second one may be related to another competing order parameter that exists well above T C and is not in direct correlation to the superconducting transition [37,38].…”
Section: Resultsmentioning
confidence: 99%
“…2) consists primarily of Fe 3d orbit als. The angular dependence of the photoelectron spectra of the cuprates between 0 and 90° has a strong dip in the middle of this range [27] (Fig. 1b), which points to anisotropic d wave superconductivity [11,12] and corresponds to hidden symmetry (D 4h ), in addition to the crystal symmetry (D 2h ) [20,21].…”
Section: Brief Survey Of Experimental Datamentioning
confidence: 96%