2017
DOI: 10.1103/physrevb.96.014517
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s+is superconductivity with incipient bands: Doping dependence and STM signatures

Abstract: Motivated by the recent observations of small Fermi energies and comparatively large superconducting gaps, present also on bands not crossing the Fermi energy (incipient bands) in iron-based superconductors, we analyze the doping evolution of superconductivity in a four-band model across the Lifshitz transition including BCS-BEC crossover effects on the shallow bands. Similar to the BCS case, we find that with hole doping the phase difference between superconducting order parameters of the hole bands change fr… Show more

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Cited by 35 publications
(36 citation statements)
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“…This should be experimentally measureable in muon-spin-rotation experiments. Note finally that qualitatively similar features should also be expected in other realizations of s + is states [10][11][12][13][14]43].…”
Section: Discussionsupporting
confidence: 77%
“…This should be experimentally measureable in muon-spin-rotation experiments. Note finally that qualitatively similar features should also be expected in other realizations of s + is states [10][11][12][13][14]43].…”
Section: Discussionsupporting
confidence: 77%
“…It would be interesting to search for doping induced modifications in the superconducting order parameter sign between the electron and hole bands. If the hole band can be brought closer to the Fermi level, predictions range from intraband s± superconductivity to time-reversal symmetry breaking s + is superconductivity, with superconducting order parameter phase differences among bands that are not multiples of π, due to the competition between Coulomb repulsion and spin fluctuations [20,42,43]. Furthermore, the presence of hedgehog spin vortex crystal in Ni doped CaKFe 4 As 4 , which could be related to the absence of glide plane [13,42,44,45], adds an interesting ingredient likely favoring unconventional superconducting properties.…”
Section: Discussionmentioning
confidence: 99%
“…The competition between those terms is responsible for the existence of the impurity-induced s + is state [10]. The s-wave states that spontaneously break the time-reversal symmetry have been a subject of much interest in recent years; see, e.g., [9][10][11][12][13][14][15][16][17]. In this work, we focus on the physics of the direct s ± to the s ++ impurity-induced crossover in an external magnetic field (denoted by the solid black line on Fig.…”
Section: Theoretical Frameworkmentioning
confidence: 99%