Application of Rapid Fluorescence Lifetime Imaging Microscopy (RapidFLIM) to Examine Dynamics of Nanoparticle Uptake in Live Cells.

A key challenge in nanomedicine stems from the continued need for a systematic understanding of the delivery of nanoparticles in live cells. Complexities in delivery are often influenced by the biophysical characteristics of nanoparticles, where even subtle changes to nanoparticle designs can alter cellular uptake, transport and activity. Close examination of these processes, especially with imaging, offers important insights that can aid in future nanoparticle design or translation. Rapid fluorescence lifetime imaging microscopy (RapidFLIM) is a potentially valuable technology for examining intracellular mechanisms of nanoparticle delivery by directly correlating visual data with changes in the biological environment. To date, applications for this technology in nanoparticle research have not been explored. A PicoQuant RapidFLIM system was used together with commercial silica nanoparticles to follow particle uptake in glioblastoma cells. Importantly, RapidFLIM imaging showed significantly improved image acquisition speeds over traditional FLIM, which enabled the tracking of nanoparticle uptake into subcellular compartments. We determined mean lifetime changes and used this to delineate significant changes in nanoparticle lifetimes (>0.39 ns), which showed clustering of these tracks proximal to both extracellular and nuclear membrane boundaries. These findings demonstrate the ability of RapidFLIM to track, localize and quantify changes in single nanoparticle fluorescence lifetimes and highlight RapidFLIM as a valuable tool for multiparameter visualization and analysis of nanoparticle molecular dynamics in live cells.

Toward single-metal-ion sensing by Förster resonance energy transfer.

Here we describe progress toward our objective of detecting single nonfluorescent hydrated metal ions. Single-ion detection represents detection and spectroscopy at the ultimate sensitivity level of approximately 1.6 x 10(-24) M. Achieving this goal would provide a breakthrough in analytical science and allow much more detailed insight into sensor-ion interaction than that available with conventional bulk detection methods. We combine recent advances in confocal microscopy with the sensitivity and the noninvasive nature of fluorescence by analyzing Förster resonance energy transfer between sensor fluorophores and transition metal ions.

Effect of pH on aqueous phenylalanine studied using a 265-nm pulsed light-emitting diode.

Recently, we described the characteristics and application of a 265-nm AlGaN light-emitting diode (LED) operated at 1-MHz repetition rate, 1.2-ns pulse duration, 1.32-microW average power, 2.3-mW peak power, and approximately 12-nm bandwidth. The LED enables the fluorescence decay of weakly emitting phenylalanine to be measured routinely in the condensed phase, even in dilute solution. For a pH range of 1-11, we find evidence for a biexponential rather than a monoexponential decay, whereas at pH 13, only a monoexponential decay is present. These results provide direct evidence for the dominance of two phenylalanine rotamers in solution with a photophysics closer to the other two fluorescent amino acids, tyrosine and tryptophan, than has previously been reported. Although phenylalanine fluorescence is difficult to detect in most proteins because of its low quantum yield and resonance energy transfer from phenylalanine to tyrosine and tryptophan, the convenience of the 265-nm LED may well take protein photophysics in new directions, for example, by making use of this resonance energy transfer or by observing phenylalanine fluorescence directly in specific proteins where resonance energy transfer is inefficient.

Single molecule level detection of allophycocyanin by surface enhanced resonance Raman scattering.

Single molecule level detection of the near-infrared fluorescent protein allophycocyanin (APC) has been achieved using surface enhanced resonance Raman scattering (SERRS). The detection limit using the peak height of the 440 cm(-1) band was 1 x 10(-13) mol l(-1), compared to 2 x 10(-12) mol l(-1) for the fluorescence peak at 660 nm.