Nanoassemblies are formed via self-assembly of ZnS capped CdSe quantum dots (QD) and perylene bisimide dyes (PBI). Upon assembly formation with functionalized dye molecules the QD photoluminescence (PL) is quenched. Quenching has been assigned partly to FRET (fluorescence resonance energy transfer) and NON-FRET processes. By means of time resolved single particle spectroscopy of immobilized QD-dye assemblies, it is demonstrated that NON-FRET processes are due to new non-radiative decay channels caused by the assembly formation process itself. Immobilized (single) assemblies exhibit the same processes as ensembles of assemblies in toluene solution. Only one dye molecule on a QD quenches the PL up to 50%, which is much stronger than is expected when replacing a volume related number of ligands. NON-FRET processes are distinct from photoinduced charge and/or energy transfer. A combination of a Stern-Volmer and FRET analysis of ensemble experiments supports the investigation of the dynamics of assembly formation at extremely low concentration ratios of PBI to QD. This allows us to distinguish between the effects of PBI and ligands on PL quenching on a single molecule level which is not possible in conventional ligand dynamic experiments.

Functional dye molecules, such as porphyrins, attached to CdSe quantum dots (QDs) through anchoring meso-pyridyl substituents, form quasi-stable nanoassemblies. This fact results in photoluminescence (PL) quenching of the QDs both due to Förster resonance energy transfer (FRET) and the formation of non-radiative surface states under conditions of quantum confinement (non-FRET). The formation process is in competition with the ligand dynamics. At least two timescales are found for the formation of the assemblies: 1) one faster than 60 s attributed to saturation of empty attachment sites and 2) one slower than 600 s, which is attributed to a reorganisation of the tri-n-octylphosphine oxide (TOPO) ligand shell. Finally, this process results in almost complete exchange of the TOPO shell by porphyrin dye molecules. Following a Stern-Volmer analysis, we established a microscopic description of PL quenching and assembly formation. Based on this formalism, we determined the equilibrium constant for assembly formation between QDs and the pyridyl-functionalised dye molecules to be K ≈ 10(5) - 10(7)  M(-1), which is several orders of magnitude larger than that of the TOPO ligands. Our results give additional insights into the non-FRET PL quenching processes involved and show that the QD surface is inhomogeneous with respect to the involved attachment and detachment processes. In comparison with other methods, such as NMR spectroscopy, the advantage of our approach is that ligand dynamics can be investigated at extremely low ratios of dye molecules to QDs.

RNA is commonly believed to undergo a number of sequential folding steps before reaching its functional fold, i.e., the global minimum in the free energy landscape. However, there is accumulating evidence that several functional conformations are often in coexistence, corresponding to multiple (local) minima in the folding landscape. Here we use the 5′-exon-intron recognition duplex of a self-splicing ribozyme as a model system to study the influence of Mg 2+ NA folding is a hierarchical process that depends on the sequential formation of secondary and tertiary structures. As the RNA phosphate-sugar backbone is negatively charged, structural compaction creates electrostatic repulsion, which must be overcome by positive charges. The majority of negative charges are nonspecifically screened by the ion atmosphere, typically a set of dynamically exchanging M + ions (1). An estimated 10-20% of negative charge is, however, compensated by M n+ that bind site-specifically to the RNA molecule, in particular, Mg 2+ (2). One RNA molecule that is known to harbor several specific M 2+ binding sites is the self-splicing group II intron Sc.ai5γ from the yeast mitochondrial cox1 (cytochrome oxidase 1) gene (3). It is one of the largest known RNA enzymes, and both its folding pathway and catalysis are strictly dependent on Mg 2+. In turn, the splicing reaction is inhibited by small amounts of Ca 2+ (4). Site specificity of the two sequential transesterfication reactions is ensured by proper base pairing between distal exon-binding sites (5′ cleavage, EBS1 and 2; 3′ cleavage, EBS3) and intron-binding sites (IBS1, 2, and 3) (5).Single-molecule Förster resonance energy transfer (smFRET), i.e., distance-dependent energy transfer between a single pair of fluorophores, is ideally suited to study the cation-dependent conformational dynamics of single RNA molecules (6, 7). If different conformations lead to distinctly different transfer efficiencies, smFRET unveils the entire folding pathway, reports on the relative occurrence of all conformations present in the ensemble, and provides detailed information on the rates at which they interconvert (7). This is important because simple two-state folding is rarely observed in experimental data (8, 9). Rather, the vast conformational space sampled by biomolecules often results not only in folding intermediates but also in kinetic traps and/or multiple native states. In an smFRET experiment, individual molecules consequently display different behaviors that may or may not persist over the observation period (10). Heterogeneity has been precedented for a number of RNA molecules, including group I introns (11, 12), the hairpin ribozyme (13-17), and RNase P RNA (18). In addition, heterogeneity has been reported for different . However, the molecular basis of the phenomenon is often enigmatic, and its quantitative characterization is challenging (21).Here we use the 5′-exon-intron recognition site of the Sc.ai5γ ribozyme to study Mg 2+ -and Ca 2+ -mediated RNA-RNA structure formation by smFRET. ...

Nanoassemblies are formed via self-assembly of ZnS capped CdSe quantum dots (QD) and perylene bisimide (PBI) dyes. Upon assembly formation the QD photoluminescence is quenched, as can be detected both via single particle detection and ensemble experiments in solution. Quenching has been assigned to FRET and NON-FRET processes. Analysis of FRET allows for a distinction between different geometries of the QD dye assemblies. Time-resolved single molecule spectroscopy reveals intrinsic fluctuations of the PBI fluorescence lifetime and spectrum, caused by rearrangement of the phenoxy side groups. The distribution of such molecular conformations and their changed dynamics upon assembly formation are discussed in the scope of FRET efficiency and surface ligand density.