Presentation Information

[PC2-05-INV]Two-dimensional superconductivity and anomalous vortex dissipation in transition metal dichalcogenide-based superlattices

*Xianhui Chen1 (1. University of Sciecne and Technology of China (China))
PDF DownloadDownload PDF

Keywords:

2D superconductivity,superconducting anisotropy,Josephson vortex

Properties of layered superconductors can vary drastically when thinned down from bulk to monolayer owing to the reduced dimensionality and weakened interlayer coupling. In transition metal dichalcogenides (TMDs), the inherent symmetry breaking effect in atomically thin crystals prompts novel states of matter such as Ising superconductivity with an extraordinary in-plane upper critical field [1,2]. We demonstrate that two-dimensional (2D) superconductivity resembling those in atomic layers but with more fascinating behaviors can be realized in the bulk crystals of new TMD-based superconductors Ba0.75ClMX2 (M = Nb, Ta; X = S, Se) [3,4]. They comprise an alternating stack of H-type MX2 layers and Ba−Cl layers (Figure 1). In all materials, intrinsic 2D superconductivity develops below a Berezinskii−Kosterlitz−Thouless transition. In particular, Ba0.75ClTaSe2 exhibits an extremely high μ0Hc2||ab ≈ 14 μ0Hp and a colossal superconducting anisotropy (Hc2||ab / Hc2ab) of ∼150. Moreover, the temperature-field phase diagram of Ba0.75ClTaSe2 under an in-plane magnetic field contains a large phase regime of vortex dissipation, which can be ascribed to the Josephson vortex motion, signifying an unprecedentedly strong fluctuation effect in TMD-based superconductors. These results provide a new path toward the establishment of 2D superconductivity and novel exotic quantum phases in bulk crystals of TMD-based superconductors.