COMMUNICATIONeither exhibit a weak chiral response or require illuminations at quite shallow angles of incidence. More importantly, because of the design complexity of the proposed chiral patterns and the enhancement mechanism being linked only to the localized mode, it is hard to tailor the chiral resonance by simply altering geometric parameters. [ 41 ] Although some pioneer work [ 35,36 ] on chiral metasurfaces linked the collective chiral responses to the propagating modes, there is still lack of clear demonstration. Consequently, the chiral responses shown in previous works were mostly spectrally fi xed, which severely limits practical applications. [ 5,22 ] In this communication, we study a novel chiral metasurface made of an array of nanoslits milled in a ≈100 nm thin gold layer on a sapphire substrate that exhibits pronounced chiral optical resonant responses from visible to near-IR frequencies which, thanks to the effect of surface lattice resonances [ 42,43 ] introduced by a propagating mode, are fi nely controllable by the tuning of both the lattice period and the length of nanoslits. Our results clearly highlight the impact of the propagating surface plasmon modes in controlling chiral responses in metamaterials and metasurfaces, and therefore, provide a new strategy for designing chiral platforms with tailored responses as needed. Furthermore, when compared to chiral patterns made of isolated metallic nanoparticles, our metamaterial, etched in a continuous metal fi lm, allows electrical conductivity across the fi lm, thus enabling applications for optoelectric devices as well.The proposed chiral pattern, a square lattice metamaterial array with unit cell period p , is illustrated in Figure 1 . Each metamolecule is made of four nanoslits of identical length a and width b separated by a gap g , in a chiral arrangement where each slit has a 90° rotation with respect to the preceding one and is aligned with its long axis to the center of the following one, in either clockwise or anticlockwise rotation, to determine the handedness of the isotropic chiral pattern. Figure 1 b,c shows scanning electron microscope (SEM) images over a magnifi ed area of a 40 × 40 µm 2 metamaterial array (50 × 50 unit cells) for the same sample design with opposite handedness ( a = 350 nm, b = 100 nm, g = 50 nm, p = 810 nm), fabricated by focus ion beam milling of the gold fi lm, while arrays with the same unit cell size and different lattice constant are also prepared.Based on the resonant profi le of a single nanoslit, the chiral confi guration will exhibit overlapping of E-fi eld and H-fi eld hot spots occurring around the four gaps, [ 6,39 ] which means that the localized plasmon mode given by the coupling between adjacent nanoslits in one unit cell contributes to the enhancement of Chirality is a key molecular structural concept and a ubiquitous phenomenon in nature that has become an increasingly signifi cant research avenue since it was introduced in the context of metamaterials. [ 1,2 ] Compared with the weak chiral opt...