Unconventional superconductivity in chiral molecule-TaS<sub>2</sub> hybrid superlattices.

Wan, Zhong; Qiu, Gang; Ren, Huaying; Qian, Qi; Li, Yaochen; Xu, Dong; Zhou, Jingyuan; Zhou, Jingxuan et al. · Nature · 2024

basic_science · Level V

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Abstract

Chiral superconductors, a unique class of unconventional superconductors in which the complex superconducting order parameter winds clockwise or anticlockwise in the momentum space<sup>1</sup>, represent a topologically non-trivial system with intrinsic time-reversal symmetry breaking (TRSB) and direct implications for topological quantum computing<sup>2,3</sup>. Intrinsic chiral superconductors are extremely rare, with only a few arguable examples, including UTe<sub>2</sub>, UPt<sub>3</sub> and Sr<sub>2</sub>RuO<sub>4</sub> (refs. <sup>4-7</sup>). It has been suggested that chiral superconductivity may exist in non-centrosymmetric superconductors<sup>8,9</sup>, although such non-centrosymmetry is uncommon in typical solid-state superconductors. Alternatively, chiral molecules with neither mirror nor inversion symmetry have been widely investigated. We suggest that an incorporation of chiral molecules into conventional superconductor lattices could introduce non-centrosymmetry and help realize chiral superconductivity<sup>10</sup>. Here we explore unconventional superconductivity in chiral molecule intercalated TaS<sub>2</sub> hybrid superlattices. Our studies reveal an exceptionally large in-plane upper critical field B<sub>c2,||</sub> well beyond the Pauli paramagnetic limit, a robust π-phase shift in Little-Parks measurements and a field-free superconducting diode effect (SDE). These experimental signatures of unconventional superconductivity suggest that the intriguing interplay between crystalline atomic layers and the self-assembled chiral molecular layers may lead to exotic topological materials. Our study highlights that the hybrid superlattices could lay a versatile path to artificial quantum materials by combining a vast library of layered crystals of rich physical properties with the nearly infinite variations of molecules of designable structural motifs and functional groups<sup>11</sup>.