Evolution of transport properties in FeSe thin flakes with thickness approaching the two-dimensional limit
C. S. Zhu, B. Lei, Z. L. Sun, J. H. Cui, M. Z. Shi, W. Z. Zhuo, X. G., Luo, and X. H. Chen

TL;DR
This study investigates how the superconducting and nematic properties of FeSe thin flakes evolve as their thickness approaches the two-dimensional limit, revealing suppressed transition temperatures, 2D superconductivity signatures, and a linear relation between $T_c$ and inverse thickness.
Contribution
It provides a systematic analysis of the evolution of superconductivity and nematicity in FeSe flakes down to bilayer, highlighting 2D superconductivity and related phenomena.
Findings
Superconducting transition temperature $T_c$ decreases with thickness.
Signatures of Berezinskii-Kosterlitz-Thouless transition observed in ultrathin flakes.
$T_c$ shows linear dependence on inverse thickness for $d \,\le\, 13$ nm.
Abstract
Electronic properties of FeSe can be tuned by various routes. Here, we present a comprehensive study on the evolution of the superconductivity and nematicity in FeSe with thickness from bulk single crystal down to bilayer ( 1.1 nm) through exfoliation. With decreasing flake thickness, both the structural transition temperature and the superconducting transition temperature are greatly suppressed. The magnetic field () dependence of Hall resistance at 15 K changes from -nonlinear to -linear behavior up to 9 T, as the thickness () is reduced to 13 nm. is linearly dependent on the inverse of flake thickness (1/) when 13 nm, and a clear drop of appears with thickness smaller than 27 nm. The - characteristic curves in ultrathin flakes reveal the signature of Berezinskii-Kosterlitz-Thouless…
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