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Recent advances in super-resolution imaging techniques, together with new fluorescent probes have enhanced our understanding of bacterial pathogenesis and their interplay within the host. In this review, we provide an overview of what these techniques have taught us about the bacterial lifestyle, the nucleoid organization, its complex protein secretion systems, as well as the secreted virulence factors.

This article reports the thermodynamics and kinetics of keto-enol tautomerization in 1, 3, 5-triazin-2, 4(1H, 3H)-dione (R) and its tautomers at D ensity F unctional T heory (DFT) – B3LYP/6-311++G (d, p) level. In the chosen system, five keto-enol tautomerization reactions are possible namely R ↔ P1 (Channel 1), R ↔ P2 (Channel 2), R ↔ P3 (Channel 3), P3 ↔ P4 (Channel 4), and P1 ↔ P4 (Channel 5). The reactant has three pathways leading to three different tautomers (P1, P2, and P3). Both P1 and P3 can tautomerize to a fourth product P4 through two additional pathways. The four tautomers namely P1, P2, P3, and P4 are defined as 6-Hydroxy-1H-[1,3,5]Triazine-2-one, 4-Hydroxy-5H-[1,3,5]Triazine-2-one, 4-Hydroxy-1H-[1,3,5]Triazine-2-one, and [1,3,5]Triazine-2,4-diol, respectively. Conventional T ransition S tate T heory (TST) calculations were carried out to determine pre-exponential factor (A) and activation energy (Ea) of all the five tautomerization reactions. One of the hydrogens bonded to the 6th carbon atom (according to IUPAC nomenclature) of the tri-heterocyclic triazine system (R) was replaced by six substituents (F, Cl, OH, NH2, CH3, and C2H5) consecutively to understand their influence on the kinetics and thermodynamics of the tautomerization processes. All substituents investigated enhances the reaction rate constants of the first channel by reducing the barrier height, for example, ortho-para directing and activating substituent NH2 reduces it by 3.55 kcal mol−1. Application of Mulliken population analysis for the distribution of π electron density indicates that the electron donating OH, NH2, and C2H5 substituents increases the stability of TS’s for the third channel by enhancing the aromaticity of triazine ring which leads to increased rate constants.

Despite significant interest in understanding the role of the local dielectric environment and lipid-bilayer fluidity/rigidity in resonance energy transfer between chromophores at lipid/water interfaces, a comprehensive approach to quantify such environmental dependence on energy transfer is missing – primarily because of the scarcity of suitable probes. Here we present the results on multi-chromophoric Forster resonance energy transfer (FRET) from a series of 4-aminophthalimide-based molecules (4AP-Cn; n = 2–10, 12) of different lipophilicity (donors), which reside at different depths across the lipid/water interfaces, to rhodamine-6G (Rh6G; acceptor) molecules that stay in a water-rich region near the lipid headgroups. We apply steady-state and time-resolved fluorescence spectroscopy, and find that multi-chromophoric FRET from the series of 4AP-Cn donors to the Rh6G acceptor occurs in a peculiar stepwise fashion at the lipid/water interface of a gel-phase (Lβ′) DPPC (1,2-dipalmitoyl-sn-glycero-3-phosphocholine) bilayer at room temperature. However, the same donor–acceptor pairs show only subtle but continuous donor-depth-dependent FRET at the lipid/water interface of a fluid-phase (Lα) DOPC (1,2-dioleoyl-sn-glycero-3-phosphocholine) bilayer. These features were found to correlate with the lipid-phase dependent local environmental polarity sensed by 4AP-Cn donors at the interfaces. Molecular dynamics (MD) simulations, combined with experimental results, show that relative depth (and angle) variation of the 4AP-Cn donors and Rh6G acceptor directly controls the FRET efficiencies through fine tuning of the emission and absorption spectra of the donors and acceptor, respectively. The results indicate that the 4AP-Cn probes are well-suited as donors for FRET studies, which allow the FRET parameters at lipid/water interfaces of gel- and fluid-phases of lipid-bilayers to be quantified and compared simultaneously.

After Salmonella is phagocytosed, it resides in an acidic vacuole. Its cytoplasm acidifies to pH 5.6; acidification activates pathogenicity island 2 (SPI-2). SPI-2 encodes a type three secretion system whose effectors modify the vacuole, driving endosomal tubulation. Using super-resolution imaging in single bacterial cells, we show that low pH induces expression of the SPI-2 SsrA/B signaling system. Single particle tracking, atomic force microscopy, and single molecule unzipping assays identified pH-dependent stimulation of DNA binding by SsrB. A so-called phosphomimetic form (D56E) was unable to bind to DNA in live cells. Acid-dependent DNA binding was not intrinsic to regulators, as PhoP and OmpR binding was not pH-sensitive. The low level of SPI-2 injectisomes observed in single cells is not due to fluctuating SsrB levels. This work highlights the surprising role that acid pH plays in virulence and intracellular lifestyles of Salmonella; modifying acid survival pathways represents a target for inhibiting Salmonella., eLife digest Salmonellae are a group of bacteria that can cause vomiting and diarrhea if we consume contaminated food. Once in the bowel, the bacteria get inside our cells, where they stay in a compartment called the vacuole. This environment is very acidic, and the inside of the microbes also becomes more acidic in response. This change helps Salmonella to switch on genes that allow them to survive and infect humans, but it is still unclear how this mechanism takes place. To investigate this question, Liew, Foo et al. harnessed a recent technique called super-resolution imaging, which lets scientists see individual molecules in a cell. First, the technique was used to count a protein called SsrB as well as the enzyme that activates it, SsrA. The role of SsrB is to bind to DNA and turn on genes involved in making proteins that help Salmonella thrive. These studies revealed that the levels of SsrA/B proteins increased three-fold in an acidic environment. Then, Liew, Foo et al. followed SsrB inside cells, knowing that fast-moving particles are free in solution, while slow-moving particles are typically bound to DNA. In acidic conditions, the proportion of SsrB bound to DNA doubled. Finally, further experiments revealed that when the environment was acidic, SsrB became five times more likely to bind to DNA. Taken together, the results suggest that acidic conditions trigger a cascade of events which switch on genetic information that allows Salmonella to survive. If SsrB could be prevented from responding to acid stress, it could potentially stop Salmonella from surviving inside host cells. This knowledge should be applied to drive new treatment strategies for Salmonella and other microbes that infect human cells.

Environment polarity and hydration at lipid/water interfaces play important roles in membrane biology, which are investigated here using a new homologous series of 4-aminophthalimide-based fluorescent molecules (4AP-Cn; n = 2–10, 12) having different lipophilicities (octanol/water partition coefficient – log P). We show that 4AP-Cn molecules probe a peculiar stepwise polarity (ENT) profile at the lipid/water interface of the gel-phase (Lβ′) DPPC (1,2-dipalmitoyl-sn-glycero-3-phosphocholine) bilayer at room temperature, which was not anticipated in earlier studies. However, the same molecules probe only a subtle but continuous polarity change at the interface of water and the fluid-phase (Lα) DOPC (1,2-dioleoyl-sn-glycero-3-phosphocholine) bilayer at room temperature. Fluorescence quenching experiments indicate that solutes with different log P values adsorb at different depths across DPPC/water and DOPC/water interfaces, which correlate with the polarity profiles observed at the interfaces. Molecular dynamics simulations performed on eight probe–lipid systems (four in each of the DPPC and DOPC bilayers – a total run of 2.6 μs) support experimental results, providing further information on the relative position and angle distributions as well as hydration of probes at the interfaces. Simulation results indicate that besides positions, probe orientations also play an important role in defining the local dielectric environment by controlling the probes' exposure to water at the interfaces especially of the gel-phase DPPC bilayer. The results suggest that 4AP-Cn probes are well suited for studying solvation properties at lipid/water interfaces of gel- and fluid-phases simultaneously.

The photophysics of green fluorescent protein (GFP) is remarkable because of its exceptional property of excited state proton transfer (ESPT) and the presence of a functional proton wire. Another interesting property of wild-type GFP is that its absorption and fluorescence excitation spectra are sensitive to the presence of polar organic solvents even at very low concentrations. Here, we use a combination of methodologies including site-specific mutagenesis, absorption spectroscopy, steady-state and time-resolved fluorescence measurements and all-atom molecular dynamics simulations in explicit solvent, to uncover the mechanism behind the unique spectral sensitivity of GFP toward organic solvents. Based on the evidences provided herein, we suggest that organic solvent-induced changes in the proton wire prevent ground state movement of a proton through the wire and thus bring about the spectral changes observed. The present study can not only help to understand the mechanism of proton transfer by further dissecting the intricate steps in GFP photophysics but also encourages to develop GFP-based organic solvent biosensors.

The fact that ubiquitous water and ions are important for biological functions of biomolecules is well established. However, understanding the dynamics of water and ions near biomolecules such as DNA, protein and phospholipid is difficult, but essential, for comprehending biomolecular functions. While significant progress has been made to apprehend the hydration structure and dynamics around proteins and phospholipids, understanding dynamics of water and ions near DNA remains challenging. Time-resolved fluorescence Stokes shift (TRFSS) experiments and molecular dynamics (MD) simulation have unraveled several new insights about perturbed water and counterion dynamics near poly-anionic DNA from femtoseconds to nanoseconds time-scales, although with debated explanations of the dispersed DNA dynamics. Here we review the advances of TRFSS experiments and MD simulation studies that unfolded several fascinating, but complex, dynamical features of perturbed water and counterions near different DNA structures in solution.

Ligand binding to minor-grooves of DNA depends on DNA-base sequence near its binding-site. However, it is not known how base-sequences affect the local solvation of ligand inside minor-grooves of DNA. Here we present a comprehensive study on sequence-dependent solvation dynamics of ligand inside duplex-DNA by measuring the static and dynamic fluorescence Stokes shifts of a popular groove-binder, DAPI, inside DNA minor-grooves created by four different sequences; d(5'-CGCGAATTCGCG-3')2, d(5'-CGCGTTAACGCG-3')2, d(5'-CGCGCAATTGCGCG-3')2, and d(5'-CGCGCTTAAGCGCG-3')2, having different sequences near DAPI-binding site. Fluorescence up-conversion and time-correlated single photon counting techniques are employed to capture the dynamic Stokes shifts of DAPI over five decades in time from 100 fs to 10 ns. We show that the ligands sense different static and dynamic solvation inside minor-grooves created by different sequences: Only subtle change in the dynamics is seen in DNA containing -AATTG-, -TTAAG-, and -AATTC- sequences, which show power-law relaxation in initial time-decades, followed by biexponential decay in nanosecond time-scales. However, changing a single base (and the complementary base) near ligand-binding site from -TTAAG- to -TTAAC- drastically induces the dynamics to follow a single power-law relaxation over the entire five decades. The observed variation of dynamics possibly relate to the local DNA motions, coupled to the hydration dynamics near the ligand-binding site.

G-quadruplex DNA (GqDNA) structures act as promising anticancer targets for small-molecules (ligands). Solvation dynamics of a ligand (DAPI: 4',6-diamidino-2-phenylindole) inside antiparallel-GqDNA is studied through direct comparison of time-resolved experiments to molecular dynamics (MD) simulation. Dynamic Stokes shifts of DAPI in GqDNA prepared in H2O buffer and D2O are compared to find the effect of water on ligand solvation. Experimental dynamics (in H2O) is then directly compared with the dynamics computed from 65 ns simulation on the same DAPI-GqDNA complex. Ligand solvation follows power-law relaxation (summed with fast exponential relaxation) from ~100 fs to 10 ns. Simulation results show relaxation below ~5 ps is dominated by water motion, while both water and DNA contribute comparably to dictate long-time power-law dynamics. Ion contribution is, however, found to be negligible. Simulation results also suggest that anomalous solvation dynamics may have origin in subdiffusive motion of perturbed water near GqDNA.

Recognition of DNA base mismatches and their subsequent repair by enzymes is vital for genomic stability. However, it is difficult to comprehend such a process in which enzymes sense and repair different types of mismatches with different ability. It has been suggested that the differential structural changes of mismatched bases act as cues to the repair enzymes, although the effect of such DNA structural changes on surrounding water and ion dynamics is inevitable due to strong electrostatic coupling among them. Thus, collective dynamics of DNA, water, and ions near the mismatch site is believed to be important for mismatch recognition and repair mechanism. Here we show that introduction of a T·T mismatch in the minor groove of DNA induces dispersed (collective) power-law solvation dynamics (of exponent ∼0.24), measured by monitoring the time-resolved fluorescence Stokes shifts (TRFSS) of two popular minor groove binders (Hoechst 33258 and DAPI) over five decades of time from 100 fs to 10 ns. The same ligands however sense different dynamics (power-law of exponent ∼0.15 or power-law multiplied with biexponential relaxation) in the minor groove of normal-DNA. The similar fluorescence anisotropy decays of ligands measured in normal- and T·T-DNA suggest that Stokes shift dynamics and their changes in T·T-DNA purely originate from the solvation process, and not from any internal rotational motion of probe-ligands. The dispersed power-law solvation dynamics seen in T·T-DNA indicate that the ligands do not sense any particular (exponential) relaxation specific to T·T wobbling and/or other conformational changes. This could be the reason why T·T mismatch is recognized by enzymes with lower efficiency compared to purine-pyrimidine and purine-purine mismatches.

G-quadruplex DNA (GqDNA) structures play an important role in many specific cellular functions and are promising anti-tumor targets for small molecules (ligands). Here, we measured the dynamic Stokes shift of a ligand (Hoechst) bound to parallel c-Myc (mPu22) GqDNA over five decades of time from 100 fs to 10 ns, and compared it with the previously reported dynamics of DAPI bound to antiparallel human telomeric (hTelo22) GqDNA (Pal et al 2015 J. Phys. Chem. Lett. 6 1754). Stokes shift data from fluorescence up-conversion and time-correlated single photon counting experiments was combined to cover the broad dynamic range. The results show that the solvation dynamics of Hoechst in parallel mPu22 GqDNA follow a power law relaxation, added to fast 2 ps exponential relaxation, from 100 fs to 10 ns, with only a subtle difference of power law exponents in the two ligand-GqDNA systems (0.06 in Hoechst-mPu22 compared to 0.16 in DAPI-hTelo22). We measured steady-state fluorescence spectra and time-resolved anisotropy decays which confirm the tight binding of Hoechst to parallel mPu22 with a binding constant of ~1 × 105 M-1. The molecular docking of Hoechst in parallel GqDNA followed by a 50 ns molecular dynamics (MD) simulation on a Hoechst-GqDNA complex reveals that Hoechst binds to one of the outer G-tetrads by end-stacking near G13 and G4, which is different from the binding site of DAPI inside a groove of antiparallel hTelo22 GqDNA. Reconciling previous experimental and simulation results, we assign the 2 ps component to the hydration dynamics of only weakly perturbed water near mPu22 and the power law relaxation to the coupled motion of water and DNA (i.e. DNA backbone, unpaired bases and loops connecting G-tetrads) which come near the Hoechst inside parallel GqDNA.

Water-in-oil microemulsion droplets (MEDs) are thermodynamically stable supramolecular structures formed in a mixture of water and oil, stabilized by surfactant layer. Here we use fluorescence correlation spectroscopy (FCS) to measure the diffusion, and the size, size distribution, and polydispersity of MEDs prepared in ternary mixtures of water/oil/sodium bis(2-ethylhexyl) sulfosuccinate (AOT) in heptane, isooctane, and nonane at (near) single droplet level. We compare FCS data directly to dynamic light scattering (DLS) data, which shows that the optical matching point (OMP) conditions of MEDs in different oils (where excess optical polarizability of droplets vanish) severely influence DLS data, while FCS extracts the accurate size, size distribution, and polydispersity of AOT-MEDs in all three oils. This suggests that extreme precaution must be taken in acquiring and explaining DLS data of MEDs in solution. FCS data show nearly identical W0-dependent (peak) size variations of AOT-MEDs in all three oils, though a subtle increase in (average) polydispersity of droplets is observed with increase in carbon chain length of oils. Establishing the accuracy of FCS data for AOT-MEDs, we further apply FCS to measure the size parameters of MEDs prepared in a quaternary mixture of water/oil/cetyltrimethylammonium bromide (CTAB)/1-butanol in hexane, heptane, and isooctane. Unlike AOT-MEDs, FCS data show substantial effect of added cosurfactant (1-butanol) and external oil on size, size distribution and polydispersity of quaternary CTAB-MEDs. Analysis of size distributions reveals large variation of polydispersity which possibly indicates the existence of larger shape heterogeneity, together with size heterogeneity, of CTAB-MEDs compared to AOT-MEDs in solution.

Time-resolved fluorescence Stokes shifts (TRFSS) of 4',6-diamidino-2-phenylindole (DAPI) inside the minor groove of DNA are measured in the presence of three different monovalent counterions: sodium (Na(+)), rubidium (Rb(+)), and tetrabutylammonium (TBA(+)). Fluorescence up-conversion and time-correlated single photon counting are combined to obtain the time-resolved emission spectra (TRES) of DAPI in DNA from 100 fs to 10 ns. Time-resolved Stokes shift data suggest that groove-bound DAPI can not sense the counterion dynamics because the ions are displaced by DAPI far from the probe-site. However, when these results are compared to the earlier base-stacked coumarin data, the same ions are found to affect the nanosecond dynamics significantly. This suggests that the ions come close to the probe-site, such that they can affect the dynamics when measured by base-stacked coumarin. These results support previous molecular dynamics (MD) simulation data of groove-bound and base-stacked probes inside DNA.

The study of ligand interaction with G-quadruplex DNA is an active research area, because many ligands are shown to bind G-quadruplex structures, showing anticancer effects. Here, we show, for the first time, how fluorescence correlation spectroscopy (FCS) can be used to study binding kinetics of ligands with G-quadruplex DNA at the single molecule level. As an example, we study interaction of a benzo-phenoxazine ligand (Cresyl Violet, CV) with antiparallel and (3 + 1) hybrid G-quadruplex structures formed by human telomeric sequence. By using simple modifications in FCS setup, we describe how one can extract the reaction kinetics from diffusion-coupled correlation curves. It is found that the ligand (CV) binds stronger, by an order of magnitude, to a (3 + 1) hybrid structure, compared to an antiparallel one. Ensemble-averaged time-resolved fluorescence experiments are also carried out to obtain the binding equilibrium constants (K) of ligand-quadruplex interactions in bulk solution for the first time, which are found to match very well with FCS results. Global analysis of FCS data provides association (k(+)) and dissociation (k(-)) rates of the ligand in the two structures. Results indicate that stronger ligand binding to the (3 + 1) hybrid structure is controlled by the dissociation rate, rather than the association rate of ligand in the quadruplexes. Circular dichroism (CD) and induced-CD spectra show that the ligand not only binds at different conformations in the quadruplexes, but also induces antiparallel structure to form a mixed-type hybrid structure in Na(+) solution. However, in K(+) solution, the ligand stabilizes the (3 + 1) hybrid structure. Molecular docking studies predict the possible differences in binding sites of the ligand inside two quadruplexes, which strongly support the experimental observations. Results suggest that different binding modes of the ligand to the quadruplex structures actually assist the alteration of structures differently.

Fluorescence correlation spectroscopy (FCS) is an ideal tool for measuring molecular diffusion and size under extremely dilute conditions. However, the power of FCS has not been utilized to its best to measure diffusion and size parameters of complex chemical systems. Here, we apply FCS to measure the size, and, most importantly, the size distribution and polydispersity of a supramolecular nanostructure (i.e., microemulsion droplets, MEDs) in dilute solution. It is shown how the refractive index mismatch of a solution can be corrected in FCS to obtain accurate size parameters of particles, bypassing the optical matching problem of light scattering techniques that are used often for particle-size measurements. We studied the MEDs of 13 different W(0) values from 2 to 50 prepared in a ternary mixture of water, sodium bis(2-ethylhexyl) sulfosuccinate (AOT), and isooctane, with sulforhodamine-B as a fluorescent marker. We find that, near the optical matching point of MEDs, the dynamic light scattering (DLS) measurements underestimate the droplet sizes while FCS estimates the accurate ones. A Gaussian distribution model (GDM) and a maximum-entropy-based FCS data fitting model (MEMFCS) are used to analyze the fluorescence correlation curves that unfold Gaussian-type size distributions of MEDs in solution. We find the droplet size varies linearly with W(0) up to ~20, but beyond this W(0) value, the size variation deviates from this linearity. To explain nonlinear variation of droplet size for W(0) values beyond ~20, we invoke a model (the coated-droplet model) that incorporates the size polydispersity of the droplets.