Nernst effect in ultrathin FeSe/SrTiO<sub>3</sub> grown by PLD
ORAL
Abstract
Ultrathin FeSe films on oxides have attracted much attention because superconductivity is enhanced by the interface effects compared to bulk form [1].
In FeSe/STO3 grown by molecular beam epitaxy, the pseudo-gap phenomenon below 70 K was reported, which was interpreted in terms of superconducting fluctuations [2]. The enhancement of superconductivity was also achieved using pulsed laser deposition (PLD) [3]. However, the superconducting fluctuations were not investigated for the PLD-grown films.
In this study, we performed the Nernst effect measurement on ultrathin FeSe/SrTiO3 grown by PLD. A 4-layer film shows a superconducting transition with a Tconset of 27 K and zero resistance below 8.4 K at 0 T. The transverse thermoelectric coefficient αxy increases below T* ~1.1×Tconset, and a peak structure is observed at low temperatures. Furthermore, magnetic field dependence of αxy changes from linear to non-linear below T*. These results indicate that superconducting fluctuations persist up to T* ~1.1×Tconset, which is similar to bulk superconductivity in Fe(Se, Te) thin films [4]. These results provide valuable insights into the nature of the interface-enhanced superconductivity in FeSe/oxide systems.
[1]. Q. Y. Wang et al., Chin. Phys. Lett. 29, 037402 (2012).
[2]. B. Faeth et al., Phys. Rev. X 11, 021054 (2021).
[3]. T. Kobayashi et al., Supercond. Sci. Technol. 35, 07LT01 (2022).
[4]. F. Nabeshima et al., Phys. Rev. B 97, 024504 (2018).
In FeSe/STO3 grown by molecular beam epitaxy, the pseudo-gap phenomenon below 70 K was reported, which was interpreted in terms of superconducting fluctuations [2]. The enhancement of superconductivity was also achieved using pulsed laser deposition (PLD) [3]. However, the superconducting fluctuations were not investigated for the PLD-grown films.
In this study, we performed the Nernst effect measurement on ultrathin FeSe/SrTiO3 grown by PLD. A 4-layer film shows a superconducting transition with a Tconset of 27 K and zero resistance below 8.4 K at 0 T. The transverse thermoelectric coefficient αxy increases below T* ~1.1×Tconset, and a peak structure is observed at low temperatures. Furthermore, magnetic field dependence of αxy changes from linear to non-linear below T*. These results indicate that superconducting fluctuations persist up to T* ~1.1×Tconset, which is similar to bulk superconductivity in Fe(Se, Te) thin films [4]. These results provide valuable insights into the nature of the interface-enhanced superconductivity in FeSe/oxide systems.
[1]. Q. Y. Wang et al., Chin. Phys. Lett. 29, 037402 (2012).
[2]. B. Faeth et al., Phys. Rev. X 11, 021054 (2021).
[3]. T. Kobayashi et al., Supercond. Sci. Technol. 35, 07LT01 (2022).
[4]. F. Nabeshima et al., Phys. Rev. B 97, 024504 (2018).
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Presenters
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Tomoki Kobayashi
Univ of Tokyo
Authors
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Tomoki Kobayashi
Univ of Tokyo
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ryo ogawa
Univ. of Tokyo
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Atsutaka Maeda
Univ of Tokyo