nanostructures as building blocks. The excitation of the light-coupled collective resonances of free electrons in plasmonic nanostructures leads to the strong lightmatter interactions at the subwavelength scale. The chiral configuration makes the interactions depend on whether the incident light has left-handed circularly polarization (LCP) or right-handed circularly polarization (RCP). Therefore, it is possible to achieve plasmonic chiral metamaterials with strongly enhanced chiroptical effects and compact size. [1,[16][17][18] A large number of plasmonic chiral metamaterials with different configurations have been demonstrated including gammadions, [19] helixes, [10] and self-assembled chiral super structures. [20] The building blocks for solid-state chiral metamaterials on substrates are either inherently chiral plasmonic nanostructures [21][22][23][24] or anisotropic achiral plasmonic nanostructures stacked into chiral structures with site-specific twists. [25][26][27][28] Fabrication of these building blocks often requires sophisticated lithographic techniques such as e-beam lithography and focused ion-beam lithography to define features at the nanoscale for targeted performances. Moreover, multistep precise alignments are needed to fabricate the metamaterials consisted of the stacked building blocks. The structural and spatial precision for the building blocks is often below 50 nm for the metamaterials working in the visible and near-infrared regimes, limiting the fabrication throughput, scalability, and reproducibility. In addition, new design and fabrication of the samples are needed to tune the chiroptical responses.Herein, we report a new type of chiral metamaterials, known as moiré chiral metamaterials (MCMs), consisted of two layers of identical achiral Au nanohole arrays stacked into moiré patterns. In contrast to the previously reported plasmonic chiral metamaterials based on local structural chirality or site-specific twisting of anisotropic components, the optical chirality of MCMs is originated from relative in-plane rotation between the lattice directions of the two identical achiral layers. The chiroptical responses of the moiré chiral metamaterials can be precisely tuned by the in-plane rotation between the two layers of nanohole arrays. Through experimental and theoretical studies, we reveal mechanism behind the chiroptical effects in the moiré chiral metamaterials. Furthermore, we apply the moiré chiral metamaterials to achieve label-free enantiodiscrimination of biomolecules and drug molecules at the picogram level. With their ultrathin thickness (≈70 nm, which is only ≈1/10 of the operation wavelength), strong chirality, and high tunability, Plasmonic chiral metamaterials are promising for applications in chiral sensors and photonic devices due to their strong optical chirality and lightmatter interactions at the subwavelength scale. However, most of current plasmonic chiral metamaterials rely on local structural chirality or site-specific symmetry breaking, which has limited their optica...