Bosons in high temperature superconductors: an experimental survey
arXiv:1105.0726 · doi:10.1088/0034-4885/74/6/066501
Abstract
We review a number of experimental techniques that are beginning to reveal fine details of the bosonic spectrum α^2F(Ω) that dominates the interaction between the quasiparticles in high temperature superconductors. Angle-resolved photo emission (ARPES) shows kinks in electronic dispersion curves at characteristic energies that agree with similar structures in the optical conductivity and tunnelling spectra. Each technique has its advantages. ARPES is momentum resolved and offers independent measurements of the real and imaginary part of the contribution of the bosons to the self energy of the quasiparticles. The optical conductivity can be used on a larger variety of materials and with the use of maximum entropy techniques reveals rich details of the spectra including their evolution with temperature and doping. Scanning tunnelling spectroscopy offers spacial resolution on the unit cell level. We find that together the various spectroscopies, including recent Raman results, are pointing to a unified picture of a broad spectrum of bosonic excitations at high temperature which evolves, as the temperature is lowered into a peak in the 30 to 60 meV region and a featureless high frequency background in most of the materials studied. This behaviour is consistent with the spectrum of spin fluctuations as measured by magnetic neutron scattering. However, there is evidence for a phonon contribution to the bosonic spectrum as well.
71 pages, 52 figures
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- Quasiparticle Interference and Strong Electron-Mode Coupling in the Quasi-One-Dimensional Bands of SrRuO
- Quasiparticle Properties of the Superconducting State of the Two Dimensional Hubbard Model
- Aspects of electron-phonon interactions with strong forward scattering in FeSe Thin Films on SrTiO substrates
- Effective SU(2) theory for the pseudogap state
- Strong-Coupling Superconductivity in NaFeCoAs: the Eliashberg Theory and Beyond
- On infrared pseudogap in cuprate and pnictide high-temperature superconductors
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