Chiral objects are defined as nonsuperimposable conformations that are mirror images of each other, much like a pair of left and right hands. In fact, the word "chiral" derives from the Greek word "χειρ" (kheir), which translates to "hand." Most biomolecules exist in only one particular conformation. For example, amino acids within large protein and peptide molecules are exclusively in the l-form (left-handed). It has long been considered that the phenomenon of homochirality (predominant occurrence of one conformation) could be linked to the origin of life. [1] These phenomena have inspired chemists and biologists to isolate, synthesize, and study the properties of chiral molecules. Research interest in chiral nanostructures has escalated rapidly since the early 2000s due to visionary reports that either predicted or demonstrated the potential applications of these materials. [2,3] In 2004, Pendry predicted that chiral metamaterials could be used to achieve negative refraction (Figure 1). [2] Following this seminal work, others demonstrated that such materials lead to circular dichroism (CD), [4] negative phase velocities, [5] and intense gyrotropy, [6] generating significant excitement within this emerging field. These properties can be harnessed to realize optical materials including "perfect lenses," [7] circular polarizers, [3] chiroptical sensors, [8] and negative refractive index materials. [9,10] In addition to these optical applications, chiral metallic nanostructures have been used for detection of biomolecular disease precursors, [11] chiral catalysis, [12] and chiral separations. [13] Many of the promising applications of chiral metallic nanostructures arise in part from their plasmonic chiroptical activity. At the nanoscale, individual metallic particles exhibit unique properties due to their high surface to volume ratio and geometric confinement of electrons. One particularly important property is the localized surface plasmon resonance (LSPR), [14] which occurs when the oscillation of surface electrons matches the frequency of incident photons. The spectral position and intensity of the LSPR depends not only on the size, shape, composition, and dielectric environment of the metallic nanoparticles (NPs) [15,16] but also on their aggregation state or assembly. [17] When metallic NPs are arranged in a chiral geometry, [18] the coupling of individual plasmons leads to collective plasmon oscillation across the entire structure. [19] Chiral NP assemblies may exhibit enhanced optical chirality in Chiral nanoparticle (NP) superstructures, in which discrete NPs are assembled into chiral architectures, represent an exciting and growing class of nanomaterials. Their enantiospecific properties make them promising candidates for a variety of potential applications. Helical NP superstructures are a rapidly expanding subclass of chiral nanomaterials in which NPs are arranged in three dimensions about a screw axis. Their intrinsic asymmetry gives rise to a variety of interesting properties, including plasmonic chir...