RESUMO
Chiroptically active, hierarchically structured materials are difficult to accurately characterize due to linear anisotropic contributions (i.e., linear dichroism (LD) and linear birefringence (LB)) and parasitic ellipticities that produce artifactual circular dichroism (CD) signals, in addition to chiral analyte contributions ranging from molecular-scale clusters to micron-sized assemblies. Recently, we have shown that CdS magic-sized clusters (MSC) can self-assemble into ordered films that have a hierarchical structure spanning seven orders of length-scale. These films have a strong CD response, but the chiral origins are obfuscated by the hierarchical architecture and LDLB contributions. Here, we derive and demonstrate a method for extracting the "pure" CD signal (CD generated by structural dissymmetry) from hierarchical MSC films and identified the chiral origin. The theory behind the method is derived using Mueller matrix and Stokes vector conventions and verified experimentally before being applied to hierarchical MSC and nanoparticle films with varying macroscopic orderings. Each film's extracted "true CD" shares a bisignate profile aligned with the exciton peak, indicating the assemblies adopt a chiral arrangement and form an exciton coupled system. Interestingly, the linearly aligned MSC film possesses one of the highest g-factors (0.05) among semiconducting nanostructures reported. Additionally, we find that films with similar electronic transition dipole alignment can possess greatly different g-factors, indicating chirality change rather than anisotropy is the cause of the difference in the CD signal. The difference in g-factor is controllable via film evaporation geometry. This study provides a simple means to measure "true" CD and presents an example of experimentally understanding chiroptic interactions in hierarchical nanostructures.
RESUMO
Solid-state ECD (ss-ECD) spectra of a model microcrystalline solid, finasteride, dispersed into a KCl pellet were recorded by using the synchrotron radiation source at the Diamond B23 beamline. Scanning a surface of 36â mm2 with a step of 0.5â mm, we measured a set of ECD imaging (ECDi) spectra very different from each other and from the ss-ECD recorded with a bench-top instrument (1â cm2 area). This is due to the anisotropic part of the ECD (ACD), which averages to zero in solution or on a large number of randomly oriented crystallites, but can otherwise be extremely large. Two-way singular value decomposition (SVD) analysis, through experimental and simulated TDDFT spectra, disclosed that the measured and theoretical principal components are in line with each other. This finding demonstrates that the observed isotropic ss-ECD spectrum is governed by the anisotropy of locally oriented crystals. It also introduces a new quality for ss-ECD measurements and opens a new future for probing and mapping chiral materials in the solid state such as active pharmaceutical ingredients (APIs).
Assuntos
Eletrônica , Anisotropia , Dicroísmo CircularRESUMO
Diatoms possess special light-harvesting proteins involved in the photoprotection mechanism called non-photochemical quenching (NPQ). These Lhcx proteins were shown to be subunits of trimeric fucoxanthin-chlorophyll complexes (FCPa) in centric diatoms, but their mode of action is still unclear. Here we investigated the influence of Fcp6, an orthologue to Lhcx1 of Thalassiosira pseudonana in the diatom Cyclotella meneghiniana, by reducing its amount using an antisense approach. Whereas the pigment interactions inside FCPa were not influenced by the presence or absence of Fcp6, as demonstrated by unaltered spectra of circular dichroism, changes could be observed on the level of thylakoids and cells in the mutants compared to WT. This fits to recent models of NPQ in diatoms, where FCP aggregation or supramolecular reorganisation is thought to be a major feature. Thus, Fcp6 (Lhcx1) appears to alter pigment-pigment interactions inside the aggregates, but not inside (un-aggregated) FCPa itself.