Observation of a ubiquitous three-dimensional superconducting gap function in optimally-doped Ba\(_{0.6}\)K\(_{0.4}\)Fe\(_2\)As\(_2\)
The iron-pnictide superconductors have a layered structureformed by stacks of FeAs planes from which the superconductivity originates. Given the multiband and quasi three-dimensional \cite{3D_SC} (3D) electronic structure of these high-temperature superconductors, knowledge of the quasi-3D supercond...
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Published in | arXiv.org |
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Main Authors | , , , , , , , , , , , , |
Format | Paper |
Language | English |
Published |
Ithaca
Cornell University Library, arXiv.org
08.03.2011
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Subjects | |
Online Access | Get full text |
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Summary: | The iron-pnictide superconductors have a layered structureformed by stacks of FeAs planes from which the superconductivity originates. Given the multiband and quasi three-dimensional \cite{3D_SC} (3D) electronic structure of these high-temperature superconductors, knowledge of the quasi-3D superconducting (SC) gap is essential for understanding the superconducting mechanism. By using the \KZ-capability of angle-resolved photoemission, we completely determined the SC gap on all five Fermi surfaces (FSs) in three dimensions on \BKFAOP samples. We found a marked \KZ dispersion of the SC gap, which can derive only from interlayer pairing. Remarkably, the SC energy gaps can be described by a single 3D gap function with two energy scales characterizing the strengths of intralayer \(\Delta_1\) and interlayer \(\Delta_2\) pairing. The anisotropy ratio \(\Delta_2/\Delta_1\), determined from the gap function, is close to the c-axis anisotropy ratio of the magnetic exchange coupling \(J_c/J_{ab}\) in the parent compound \cite{NeutronParent}. The ubiquitous gap function for all the 3D FSs reveals that pairing is short-ranged and strongly constrain the possible pairing force in the pnictides. A suitable candidate could arise from short-range antiferromagnetic fluctuations. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.1006.3958 |