STM and Nernst measurements on tetragonal and orthogonal phase of Fe(Se<sub>1-x</sub>S<sub>x</sub>)
ORAL
Abstract
The crossover from the Bardeen-Cooper-Schrieffer (BCS) state for weakly paired fermions to the Bose Einstein condensation (BEC) state of tightly-bound pairs has attracted much attention as a new paradigm of superconductivity. In the BCS-BEC crossover regime, exotic phenomena, such as pseudogap formation owing to preformed pairs above superconducting transition temperature Tc, have been predicted.
It has been reported that multiband iron-based superconductor FeSe with the small Fermi energies is located at the BCS-BEC crossover regime. Moreover, very recent heat capacity and ARPES measurements have suggested a possibility that the tetragonal phase of Fe(Se1-xSx) (x > 0.17) is located at the state closer to the BEC limit. Pairing fluctuation and pseudogap formation above Tc, however, have not been reported so far.
In this study, we perform STM and Nernst measurements on FeSe0.87S0.13 and FeSe0.75S0.25, which are in the orthogonal and tetragonal phases, respectively. In our Nernst measurements, well exceeding Gaussian fluctuations are observed above Tc in FeSe0.75S0.25, while pseudogap formation is not observed by the STM measurements. We will discuss the present results in terms of the BCS-BEC crossover in multiband superconducting systems.
It has been reported that multiband iron-based superconductor FeSe with the small Fermi energies is located at the BCS-BEC crossover regime. Moreover, very recent heat capacity and ARPES measurements have suggested a possibility that the tetragonal phase of Fe(Se1-xSx) (x > 0.17) is located at the state closer to the BEC limit. Pairing fluctuation and pseudogap formation above Tc, however, have not been reported so far.
In this study, we perform STM and Nernst measurements on FeSe0.87S0.13 and FeSe0.75S0.25, which are in the orthogonal and tetragonal phases, respectively. In our Nernst measurements, well exceeding Gaussian fluctuations are observed above Tc in FeSe0.75S0.25, while pseudogap formation is not observed by the STM measurements. We will discuss the present results in terms of the BCS-BEC crossover in multiband superconducting systems.
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Presenters
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Masahiro Haze
- Department of Physics, Kyoto University