Issue |
EPL
Volume 87, Number 1, July 2009
|
|
---|---|---|
Article Number | 17007 | |
Number of page(s) | 6 | |
Section | Condensed Matter: Electronic Structure, Electrical, Magnetic and Optical Properties | |
DOI | https://doi.org/10.1209/0295-5075/87/17007 | |
Published online | 24 July 2009 |
Possible strong electron-lattice interaction and giant magneto-elastic effects in Fe-pnictides
1
Goethe-University Frankfurt, Theoretical Physics - 60054 Frankfurt/Main, Germany, EU
2
Goethe-University Frankfurt, Institute of Physics - 60054 Frankfurt/Main, Germany, EU
Corresponding author: kulic@th.physik.uni-frankfurt.de
Received:
2
May
2009
Accepted:
25
June
2009
The possibility for an appreciable many-body contribution to the electron-phonon interaction (EPI) in Fe-pnictides is discussed in the model where EPI is due to the electronic polarization of As-ions. The polarization induced EPIpol potential Vep is large for vibrations of the As-ions and depends strongly on the As-Fe distance d, i.e. Vep ~ d-4. The EPIpol coupling is much larger than the one obtained in the LDA band structure calculations, with
(~16 eV/Å)
( < 1 eV/Å) and the bare pairing EPIpol coupling constant
~ 1. It contributes significantly to the intra-band s-wave pairing and an appreciable positive As-isotope effect in the superconducting critical temperature is expected. In the Fe-breathing mode the linear (in the Fe-displacements) EPIpol coupling vanishes, while the non-linear (quadratic) one is very strong. The part of the EPIpol coupling, which is due to the “potential" energy (the Hubbard U) changes, is responsible for the giant magneto-elastic effects in MFe2As2, M = Ca, Sr, Ba since it gives much larger contribution to the magnetic pressure than the band structure effects do. This mechanism is contrary to the LDA prediction where the magneto-elastic effects are due to the “kinetic" energy effects, i.e. the changes in the density of states by the magneto-elastic effects. The proposed
is expected to be operative (and strong) in other Fe-based superconductors with electronically polarizable ions such as Se, Te, S etc., and in high-temperature superconductors due to the polarizability of the O2--ions.
PACS: 74.25.Jb – Electronic structure / 74.25.Kc – Phonons / 74.70.Dd – Ternary, quaternary, and multinary compounds (including Chevrel phases, borocarbides, etc.)
© EPLA, 2009
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