A Common Thread
arXiv:1002.2413 · doi:10.1016/j.physc.2010.01.004
Abstract
The structures, the phase diagrams, and the appearance of a neutron resonance in the superconducting state provide phenomenological evidence which relate the heavy fermion, cuprate and Fe superconductors. Single- and multi-band Hubbard models have been found to describe a number of the observed properties of these materials so that it is reasonable to examine the origin of the pairing interaction in these models. Here based on the experimental phenomenology and studies of the momentum and frequency dependence of the pairing interaction for Hubbard-like models, we suggest that spin-fluctuation mediated pairing is the common thread linking this broad class of superconducting materials.
This work arose from an invitation to present an overview regarding "the mechanism of high temperature superconductivity including the cuprates and Fe- pnictides" at the 9th International Conference on Materials and Mechanisms of Superconductivity held in Tokyo (September 7-12, 2009)
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- Resilience of d-wave superconductivity to nearest-neighbor repulsion
- Electronic structure, disconnected Fermi surfaces and antiferromagnetism in the layered pnictide superconductor NaBaTiSbO
- Thermal expansion and Grüneisen parameters of Ba(Fe1-xCox)2As2 - a thermodynamic quest for quantum criticality
- Observing the origin of superconductivity in quantum critical metals
- Temperature-dependent transformation of the magnetic excitation spectrum on approaching superconductivity in Fe1-x (Ni/Cu)x Te0.5 Se0.5
- Antagonistic effects of nearest-neighbor repulsion on the superconducting pairing dynamics in the doped Mott insulator regime
- Materials and mechanisms of hole superconductivity
- Quantum phase transitions of antiferromagnets and the cuprate superconductors
- Revealing the degree of magnetic frustration by non-magnetic impurities
- Oxygen hole content, charge-transfer gap, covalency, and cuprate superconductivity
- Comments on the d-wave pairing mechanism for cuprate high superconductors: Higher is different?