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$$^{57}$$Fe nuclear resonant inelastic scattering of iron based superconductor, FeTe$$_x$$Se$$_{1-x}$$

Kurokuzu, Masayuki*; Kitao, Shinji*; Kobayashi, Yasuhiro*; Saito, Makina*; Masuda, Ryo; Mitsui, Takaya; Yoda, Yoshitaka*; Seto, Makoto*

FeTe$$_x$$Se$$_{1-x}$$ consists of only the superconducting layer of iron and chalcogenides and is one of the simplest iron-based superconductor. We measured the nuclear resonant inelastic scattering by $$^{57}$$Fe in FeTe$$_{0.5}$$Se$$_{0.5}$$ and FeTe$$_{0.9}$$, to observe the temperature dependence of their phonon density of states (PDOS); FeTe$$_{0.5}$$Se$$_{0.5}$$ has the highest superconducting temperature (T$$_c$$) among FeTe$$_x$$Se$$_{1-x}$$ and the non-superconducting FeTe$$_{0.9}$$ is the base material of FeTe$$_x$$Se$$_{1-x}$$. The difference between the PDOS of FeTe$$_{0.5}$$Se$$_{0.5}$$ at temperatures below and above T$$_c$$ is unclear. This indicates the phonons are not the main contribution to the superconductivity. On the other hand, the PDOS of FeTe$$_{0.9}$$ changes depending on temperature and this change is understood by the results of the structural phase transition.

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