Herein we report the effect of different nucleobase pair compositions on the association-induced fluorescence enhancement property of Thioflavin T (ThT), upon binding with 20 base pair long double-stranded DNA (dsDNA). Analysis of binding and decay constants along with the association (K ass ) and dissociation (K diss ) rate constants obtained from the fluctuation in the fluorescence intensity of ThT after binding with different DNA revealed selective affinity of ThT toward AT-rich dsDNA. Molecular docking also substantiates the experimental results. We also observed that addition of orange-emitting ethidium bromide (EtBr) to cyan-emitting ThT−DNA complexes leads to bright white light emission (WLE) through Forster resonance energy transfer. Additionally, the emission of white light is far greater in the case of intra-DNA strands. Besides endorsing the binding insights of ThT to AT-rich dsDNA, the present investigations open a new perspective for realizing promising WLE from two biomarkers without labeling the DNA.

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Structure, activity, and dynamics of a plasma protein, human serum albumin (HSA), inside a crowded environment of F127 gel are studied by circular dichroism (CD), fluorescence correlation spectroscopy (FCS), and picosecond time-resolved fluorescence spectroscopy. For this purpose, the protein is covalently labeled by a maleimide dye, 7-(diethylamino)-3-(4-maleimidylphenyl)-4-methyl-coumarin (CPM). The circular dichroism (CD) spectra suggest that the protein is more structured in the gel reflecting about the biological activities of the protein. FCS results demonstrate that compared to that in bulk water (buffer solution), translational diffusion is about 59 times slower inside the F127 gel. This indicates higher translational friction (viscosity) sensed by the probe (CPM). On the contrary, rotational relaxation (and hence, rotational friction) is more or less similar in F127 gel and in bulk water. FCS results further indicate that the time scales of conformational relaxation of the protein are substantially slow inside the crowded environment of F127 gel. The fast component of conformational relaxation is retarded by ∼55 times, and the slow component by ∼20 times. Fluorescence maximum of CPM bound to HSA show a ∼5 nm red shift, implying that the microenvironment of the probe, CPM, is more polar inside the gel. Solvation dynamics of CPM-labeled HSA inside the gel (⟨τ s ⟩ ∼ 300 ps) is faster compared to that for the protein in bulk water (⟨τ s ⟩ ∼ 600 ps).

Sub-nanomolar selective detection of Hg(ii) ions by protein (Human Serum Albumin, HSA) templated gold nanoclusters (AuNCs), both in in vitro as well as in vivo environments and specific endocytose behaviour towards breast cancer (BC) cell lines.

Luminescent metal nanoclusters (NCs) have been established as the next-generation fluorophores. The biocompatible and non-toxic nature, along with excellent chemical- and photo-stability render them to find applications in multi-disciplinary areas....

In this work, we propose a new analysis of the time resolved emission spectra of a photo‐acid, HA, pyranine (8‐hydroxypyrene‐1,3,6‐trisulphonic acid, HPTS) based on time resolved area normalized emission spectra (TRANES). Presence of an isoemissive point in TRANES confirms the presence of two emissive species (HA and A−) inside the system in bulk water and inside a co‐polymer hydrogel [F127, (PEO)100–(PPO)70–(PEO)100]. We show that following electronic excitation, the local pH around HPTS, is much lower than the bulk pH presumably because of ejection of proton from the photo‐acid in the excited state. With increase in time, the local pH increases and reaches the bulk value. We further, demonstrate that the excited state pKa of HPTS may be estimated from the emission intensities of HA and A− at long time. The time constant for time evolution of pH is ∼630 ps in water, ∼1300 ps in F127 gel and ∼4700 ps in CTAB micelle. The location and local viscosity sensed by the probe is ascertained using fluorescence correlation spectroscopy (FCS) and fluorescence anisotropy decay. The different values of the local viscosity reported by these two methods are reconciled.

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