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Physical Review B 85 (2012) 064519
Anomalous dependence of c-axis polarized Fe B1g phonon mode with Fe and Se concentrations in Fe1+yTe1−xSex
Pierre Toulemonde 1, A. Subedi 2, Y.J. Um 3, A.Y. Ganin 4, L. Boeri 5, M. Rahlenbeck 4, Y. Liu 4, C. T. Lin 6, S.J.E. Carlsson 1, André Sulpice 1, M.J. Rosseinsky 2, B. Keimer 7, Mathieu Le Tacon 4
(27/02/2012)

We report on an investigation of the lattice dynamical properties in a range of Fe1+yTe1−xSex compounds, with special emphasis on the c-axis polarized vibration of Fe with B1g symmetry, a Raman active mode common to all families of Fe-based superconductors. We have carried out a systematic study of the temperature dependence of this phonon mode as a function of Se x and excess Fe y concentrations. In parent compound Fe1+yTe, we observe an unconventional broadening of the phonon between room temperature and magnetic ordering temperature TN. The situation smoothly evolves toward a regular anharmonic behavior as Te is substituted for Se and long-range magnetic order is replaced by superconductivity. Irrespective to Se contents, excess Fe is shown to provide an additional damping channel for the B1g phonon at low temperatures. We performed density functional theory ab initio calculations within the local density approximation to calculate the phonon frequencies, including magnetic polarization and Fe nonstoichiometry in the virtual crystal approximation. We obtained a good agreement with the measured phonon frequencies in the Fe-deficient samples, while the effects of Fe excess are poorly reproduced. This may be due to excess Fe-induced local magnetism and low-energy magnetic fluctuations that cannot be treated accurately within these approaches. As recently revealed by neutron scattering and muon spin rotation studies, these phenomena occur in the temperature range where anomalous decay of the B1g phonon is observed and suggests a peculiar coupling of this mode with local moments and spin fluctuations in Fe1+yTe1−xSex.
1 :  Institut Néel (NEEL)
CNRS : UPR2940 – Université Joseph Fourier - Grenoble I – Institut National Polytechnique de Grenoble (INPG)
2 :  Max-Planck-Institut für Festkörperforschung
Max-Planck-Institut
3 :  Max-Planck-Institut für Festkörperforschung
Max-Planck-Institut
4 :  Max-Planck-Institut für Festkörperforschung
Max-Planck-Institut
5 :  Max-Planck-Institut für Festkörperforschung
Max-Planck-Institut für Festkörperforschung
6 :  Max-Planck-Institut for Solid State Research (MPI/FKF)
Max-Planck-Institut
7 :  Max-Planck-Institut für Festkörperforschung
Max-Planck-Institut
SPMCE
Supra
Physique/Matière Condensée/Supraconductivité
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Fe1_yTeSe_Raman_resub.pdf(1.6 MB)

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