Density of Phonon States in Superconducting FeSe as a Function of Temperature and Pressure
arXiv:1004.2007 · doi:10.1103/PhysRevB.81.184510
Abstract
The temperature and pressure dependence of the partial density of phonon states of iron atoms in superconducting Fe1.01Se was studied by 57Fe nuclear inelastic scattering (NIS). The high energy resolution allows for a detailed observation of spectral properties. A sharpening of the optical phonon modes and shift of all spectral features towards higher energies by ~4% with decreasing temperature from 296 K to 10 K was found. However, no detectable change at the tetragonal - orthorhombic phase transition around 100 K was observed. Application of a pressure of 6.7 GPa, connected with an increase of the superconducting temperature from 8 K to 34 K, results in an increase of the optical phonon mode energies at 296 K by ~12%, and an even more pronounced increase for the lowest-lying transversal acoustic mode. Despite these strong pressure-induced modifications of the phonon-DOS we conclude that the pronounced increase of Tc in Fe1.01Se with pressure cannot be described in the framework of classical electron-phonon coupling. This result suggests the importance of spin fluctuations to the observed superconductivity.
References in corpus (19)
- Superconductivity at 38 K in the iron arsenide (Ba1-xKx)Fe2As2
- Superconductivity at 43 K in Samarium-arsenide Oxides
- Superconductivity at 36 K in beta-Fe1.01Se with the compression of the interlayer separation under pressure
- Density functional study of FeS, FeSe and FeTe: Electronic structure, magnetism, phonons and superconductivity
- Structural and magnetic phase diagram of CeFeAsO1-xFx and its relationship to high-temperature superconductivity
- Superconductivity at 27 K in tetragonal FeSe under high pressure
- Extreme Sensitivity of Superconductivity to Stoichiometry in FeSe (Fe1+dSe)
- Is LaOFFeAs an electron-phonon superconductor ?
- Pressure evolution of low-temperature crystal structure and bonding of 37 K FeSe superconductor
- The Structural Phase Transition in FeSe (Fe1+dSe)
- Why Does Undoped FeSe Become A High Tc Superconductor Under Pressure?
- Structure and superconductivity of LiFeAs
- High - Temperature Superconductivity in Iron Based Layered Compounds
- Synthesis, crystal structure and chemical stability of the superconductor FeSe_{1-x}
- Superconducting and normal phases of FeSe single crystals at high pressure
- Raman scattering study of (KSr)FeAs ( = 0.0, 0.4)
- Neutron scattering Measurements of the phonon density of states of FeSe superconductors
- Moessbauer spectroscopy evidence for the lack of iron magnetic moment in superconducting FeSe
- Resistivity saturation in PrFeAsOF superconductor: An evidence of strong electron-phonon coupling
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- Lattice Dynamics of Ultrathin FeSe Films on SrTiO3
- A first-principles study of the electronic structure of Iron-Selenium; Implications for electron-phonon superconductivity
- Soft and Isotropic Phonons in PrFeAsO_{1-y}
- Correlation Driven Phonon Anomalies in Bulk FeSe
- Intercalation effect on hyperfine parameters of Fe in FeSe superconductor with Tc = 42 K
- On the phonon dispersion relation of single-crystalline --FeSe
- Probing the direct factor for superconductivity in FeSe-Based Superconductors by Raman Scattering
- The Superconducting Transition Temperatures of Fe1+xSe1--y, Fe1+xSe1--yTey and (K/Rb/Cs)zFe2--xSe2
- Pressure effect on superconductivity in FeSe0.5Te0.5
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