Two-Dimensional Superconductivity and Anomalous Vortex Dissipation in Newly Discovered Transition Metal Dichalcogenide-Based Superlattices

Abstract

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 inplane upper critical field. Here, we demonstrate that twodimensional (2D) superconductivity resembling those in atomic layers but with more fascinating behaviors can be realized in the bulk crystals of two new TMD-based superconductors Ba 0.75 ClTaS 2 and Ba 0.75 ClTaSe 2 with superconducting transition temperatures 2.75 and 1.75 K, respectively. They comprise an alternating stack of H-type TMD layers and Ba−Cl layers. In both materials, intrinsic 2D superconductivity develops below a Berezinskii−Kosterlitz−Thouless transition. The upper critical field along the ab plane (H c ab 2 || ) exceeds the Pauli limit (μ 0 H p ); in particular, Ba 0.75 ClTaSe 2 exhibits an extremely high H c ab 0 2 || ≈ 14 μ 0 H p and a colossal superconducting anisotropy (H c ab 2 || /H c ab 2 ) of ∼150. Moreover, the temperature-field phase diagram of Ba 0.75 ClTaSe 2 under an inplane 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. Our results provide a new path toward the establishment of 2D superconductivity and novel exotic quantum phases in bulk crystals of TMD-based superconductors.