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Orbital selective spin excitations and their impact on superconductivity of LiFe1-xCoxAs
We use neutron scattering to study spin excitations in single crystals of LiFe\(_{0.88}\)Co\(_{0.12}\)As, which is located near the boundary of the superconducting phase of LiFe\(_{1-x}\)Co\(_{x}\)As and exhibits non-Fermi-liquid behavior indicative of a quantum critical point. By comparing spin exc...
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Published in: | arXiv.org 2016-06 |
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Main Authors: | , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | We use neutron scattering to study spin excitations in single crystals of LiFe\(_{0.88}\)Co\(_{0.12}\)As, which is located near the boundary of the superconducting phase of LiFe\(_{1-x}\)Co\(_{x}\)As and exhibits non-Fermi-liquid behavior indicative of a quantum critical point. By comparing spin excitations of LiFe\(_{0.88}\)Co\(_{0.12}\)As with a combined density functional theory (DFT) and dynamical mean field theory (DMFT) calculation, we conclude that wave-vector correlated low energy spin excitations are mostly from the \(d_{xy}\) orbitals, while high-energy spin excitations arise from the \(d_{yz}\) and \(d_{xz}\) orbitals. Unlike most iron pnictides, the strong orbital selective spin excitations in LiFeAs family cannot be described by anisotropic Heisenberg Hamiltonian. While the evolution of low-energy spin excitations of LiFe\(_{1-x}\)Co\(_x\)As are consistent with electron-hole Fermi surface nesting condition for the \(d_{xy}\) orbital, the reduced superconductivity in LiFe\(_{0.88}\)Co\(_{0.12}\)As suggests that Fermi surface nesting conditions for the \(d_{yz}\) and \(d_{xz}\) orbitals are also important for superconductivity in iron pnictides. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.1606.00727 |