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Evidence for a preformed Cooper pair model in the pseudogap spectra of a Ca(10)(Pt(4)As(8))(Fe(2)As(2))(5) single crystal with a nodal superconducting gap
For high-T(c) superconductors, clarifying the role and origin of the pseudogap is essential for understanding the pairing mechanism. Among the various models describing the pseudogap, the preformed Cooper pair model is a potential candidate. Therefore, we present experimental evidence for the prefor...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6408529/ https://www.ncbi.nlm.nih.gov/pubmed/30850717 http://dx.doi.org/10.1038/s41598-019-40528-3 |
Sumario: | For high-T(c) superconductors, clarifying the role and origin of the pseudogap is essential for understanding the pairing mechanism. Among the various models describing the pseudogap, the preformed Cooper pair model is a potential candidate. Therefore, we present experimental evidence for the preformed Cooper pair model by studying the pseudogap spectrum observed in the optical conductivity of a Ca(10)(Pt(4)As(8))(Fe(2)As(2))(5) (T(c) = 34.6 K) single crystal. We observed a clear pseudogap structure in the optical conductivity and observed its temperature dependence. In the superconducting (SC) state, one SC gap with a gap size of Δ = 26 cm(−1), a scattering rate of 1/τ = 360 cm(−1) and a low-frequency extra Drude component were observed. Spectral weight analysis revealed that the SC gap and pseudogap are formed from the same Drude band. This means that the pseudogap is a gap structure observed as a result of a continuous temperature evolution of the SC gap observed below T(c). This provides clear experimental evidence for the preformed Cooper pair model. |
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