The effects of ligand substitution and deuteriation on the spectroscopic and photophysical properties of [Ru(LL)(CN)4]2- complexes.

The spectroscopic characterisation of a series of [Ru(LL)(CN)(4)](2-) complexes, where LL = 1,10-phenanthroline (phen) and its methyl- and phenyl-substituted derivatives and several deuteriated isotopologues are reported. The optical and vibrational properties of these complexes are compared with that of the series of 2,2'-bipyridine (bipy) derivatives and analogous [Ru(LL)(3)](2+) complexes. It has been demonstrated that substitution at the 4,4' positions of bipy and 4,7-positions of phen by electron donating (CH(3)) and withdrawing (C(6)H(5), COO(-)) groups induces a pronounced blue and red shift, respectively, in the lowest energy (1)MLCT absorption band of [Ru(LL)(CN)(4)](2-). The energy of the emission originating from the (3)MLCT excited state is found to be dependant on the nature of the vibrational modes of the aromatic rings and the electron donating and/or withdrawing properties of the substituents. Single-mode Franck-Condon analysis indicates that methyl substitution leads to a significant increase in the Huang-Rhys factor (S(M)), while phenyl substitution results in a decrease in S(M) for both series (bipy and phen) of complexes. The rate of non-radiative (k(nr)) and radiative decay (k(ph)) to the ground state and the parameters of thermally activated deactivation pathways (A(4th), DeltaE(4th) and A(dd), DeltaE(dd)) were estimated from the temperature dependence of luminescence quantum yields and lifetimes. It has been demonstrated that the non-radiative decay rate and the temperature dependent decay processes are more efficient for bipy complexes than for phen derivatives due to the rigidity of the latter ligand.     

Influence of alkyl group on amide nitrogen atom on fluorescence quenching of tyrosine amide and N-acetyltyrosine amide

The steady-state and time-resolved fluorescence spectroscopy was applied to determine the influence of an alkyl substituent(s) (methyl or ethyl, n-propyl, iso-propyl, n-butyl, sec-butyl, or t-butyl) on amide nitrogen atom on photophysical properties of tyrosine and N-acetyltyrosine amides in water. Generally, the amide group strongly quenches the fluorescence of tyrosine, however, the size and number of substituents on amide nitrogen atom modify the quenching process only in small degree. The fluorescence intensity decays of all amides studied are bi-exponential. The contribution of both components (alphai) to the fluorescence decay undergoes irregular change. An introduction of alkyl substituent on amide nitrogen atom causes an increase of the fluorescence lifetime of tyrosine derivative compared to the unsubstituted amide for both N-acetyltyrosine and tyrosine with the protonated amino group. Calculated, basing on the fluorescence quantum yield (QY) and average lifetime, the radiative rate constants (kf) are similar, which indicates that the substituent(s) does not have substantial influence on radiative process of the deactivation of the excited state of the phenol chromophore for all compounds studied regardless the amino group status as well as the number and type of substituent (linear or branched). The comparison of the ground-state rotamer populations of tyrosine amides and N-acetyltyrosine amides with different alkyl substituent on amide nitrogen atom obtained from 1H NMR with the value of pre-exponential factors indicates that not the rotamer populations, but specific hydration of a whole molecule of the amino acid including chromophore and amino acid moiety, seems to be the main reason of the heterogenous fluorescence intensity decay of tyrosine derivatives.     

Photophysical properties of 2-amino-9,10-anthraquinone: evidence for structural changes in the molecule with solvent polarity.

The photophysical properties of 2-amino-9,10-anthraquinone (2AAQ) have been investigated in different solvents and solvent mixtures and correlated with the Lippert-Mataga solvent polarity parameter, Deltaf. In the low solvent polarity region with Deltaf < ca. 0.1, the dye shows unusually high fluorescence quantum yields (Phif) and lifetimes (tauf) in comparison to those in other solvents of medium to high polarities. Similarly, the radiative rate constants (kf) are relatively lower and the non-radiative rate constants (knr) are relatively higher in the low polarity solvents in comparison to those in the medium to high polarity solvents. The current results have been rationalized assuming that the dye adopts different structural forms below and above the Deltaf value of approximately 0.1. It is inferred that in the low solvent polarity region the dye exists in a non-planar structure, with its 2-NH2 plane away from that of the 9,10-anthraquinone moiety in the ground state. In solvents of medium to high polarities, the dye exists in a polar intramolecular charge transfer (ICT) structure, where the amino lone pair of the 2-NH2 group is in strong resonance with the anthraquinone pi-cloud in the ground state. In all the solvents, however the dye is inferred to exist in the ICT structure in its excited (S1) state. Supportive evidence for the above hypothesis has been obtained from the solvent polarity effect on the Stokes' shifts for the dye. Quantum chemical studies on the structures of 2AAQ dye in the gas phase also give qualitative support for the inferences drawn from the photophysical properties of the dye in different solvents.     

pH-dependence of photo-induced electron transfer in zinc-substituted sperm whale myoglobin

The electron transfer between the excited triplet state of zinc-substituted sperm whale myoglobin and Cu2+ has been studied by following the decay rate of delayed fluorescence. The Cu2+ bound on the surface of the myoglobin molecule are efficient quenchers of the excited electron state of Zn-myoglobin. Two bimolecular rate constants of quenching (KQ) for every pH investigated have been calculated. The pH-dependence of KQ1 indicates that the protonation of one amino acid residue (His-GH1 (119] is important for the process. Our results support the idea of the common nature of the mechanism of quenching by Cu2+ and oxidation of oxymyoglobin by Cu2+.     

Relation between the secondary structure of carbohydrate residues of alpha1-acid glycoprotein (orosomucoid) and the fluorescence of the protein

We studied in this work the relation that exists between the secondary structure of the glycans of alpha(1)-acid glycoprotein and the fluorescence of the Trp residues of the protein. We calculated for that the efficiency of quenching and the radiative and non-radiative constants. Our results indicate that the glycans display a spatial structure that is modified upon asialylation. The asialylated conformation is closer to the protein matrix than the sialylated form, inducing by that a decrease in the fluorescence parameters of the Trp residues. In fact, the mean quantum yield of Trp residues in sialylated and asialylated alpha(1)-acid glycoprotein are 0.0645 and 0.0385, respectively. Analysis of the fluorescence emission of alpha(1)-acid glycoprotein as the result of two contributions (surface and hydrophobic domains) indicates that quantum yields of both classes of Trp residues are lower when the protein is in the asialylated form. Also, the mean fluorescence lifetime of Trp residues decreases from 2.285 ns in the sialylated protein to 1.948 ns in the asialylated one. The radiative rate constant k(r) of the Trp residues in the sialylated alpha(1)-acid glycoprotein is higher than that in the asialylated protein. Thus, the carbohydrate residues are closer to the Trp residues in the absence of sialic acid. The modification of the spatial conformation of the glycans upon asialylation is confirmed by the decrease of the fluorescence lifetimes of Calcofluor, a fluorophore that binds to the carbohydrate residues. Finally, thermal intensity quenching of Calcofluor bound to alpha(1)-acid glycoprotein shows that the carbohydrate residues have slower residual motions in the absence of sialic acid residues.     

Photocyclization of 2-vinyldiphenylacetylenes and behavior of the isonaphthalene intermediates.

The conformation, electronic structure, spectroscopy, and unimolecular photoisomerization of 2-vinyldiphenylacetylene and two derivatives have been investigated. 2-Vinyldiphenylacetylene exists predominantly in a planar anti conformation. Introduction of an alpha-methyl substituent results in increased phenyl-vinyl dihedral angles for both syn and anti conformers, whereas a cyclic analog is constrained to a syn conformation with a large phenyl-vinyl dihedral angle. All three molecules undergo photocyclization to yield unstable cyclic allene (isonaphthalene) intermediates which undergo further reactions leading to stable products. Both the photocyclization process and behavior of the allene intermediate are dependent upon ground state conformation. The photophysical behavior of the 2-vinyl derivative, namely its short singlet lifetime and low fluorescence quantum yield, is similar to that of diphenylacetylene. It also has a low quantum yield for photocyclization. The 2-isopropenyl derivative and conformationally locked cyclic analog have relatively long singlet lifetimes and large quantum yields for fluorescence and cyclization. The difference in excited state behavior of the planar 2-vinylacetylene and its non-planar analogs is attributed to the effect of the phenyl-vinyl dihedral angle on the barriers for activated decay of the linear singlet state. However, the behavior of the 2-isopropenyl derivative does not appear to be dependent upon ground state conformation (synvs.anti). The cyclic allene intermediates undergo sequential protonation-deprotonation in methanol solution to yield stable products. The 2-vinyl derivative yields only the fully aromatized 2-phenylnaphthalene. However, the 2-isopropenyl and cyclic derivatives yield mixtures of fully and partially aromatized products. Preferential formation of the partially aromatized products is attributed to a stereoelectronic effect on the deprotonation step. In diethyl ether solution only the fully aromatized product is formed via a free radical mechanism.     

Positional effects of the hydroxy substituent on the photochemical and photophysical behavior of 3- and 4-hydroxystilbene.

The photophysical and photochemical behavior of meta- and para-hydroxy- and methoxystilbene are reported and compared to the aminostilbenes. Absorption spectra of all four studied compounds in organic solution display a featureless, intense long-wavelength absorption band around 300 nm. In basic aqueous solution, meta-hydroxystilbene displays a less intense band with a long-wavelength shoulder, a consequence of configuration interaction from the O(-) substituent. Emission from the meta-substituted stilbenes is much stronger than from the para isomers, with an especially large effect for the hydroxystilbenes in solvents that are good hydrogen bond acceptors. Emission from the hydroxystilbenes is weak in aqueous solution, and even weaker in basic solution, a consequence of facile nonradiative decay. The excited state lifetimes of the meta isomers are longer than those with para substituents. Ground and excited state acidity constants are reported for the hydroxystilbenes. In the ground state, the para derivative is an order of magnitude more acidic than the meta isomer, however, its short excited state lifetime precludes excited state deprotonation. In contrast, 3-hydroxystilbene does exhibit deprotonation in its excited state.     

Solvatochromic study of 3‐N‐(N′‐methylacetamidino)benzanthrone and its interaction with dopamine by the fluorescence quenching mechanism

The change in photophysical properties of the organic molecule due to solvatochromic effect caused by different solvent environments at room temperature gives information about the dipole moments of 3‐N‐(N′‐methylacetamidino)benzanthrone (3‐MAB). The quantum yield, fluorescence lifetime of 3‐MAB was measured in different solvents to calculate radiative and non‐radiative rate constants. The results revealed that the excited state dipole moment (μ_e) is relatively larger compared to the ground state dipole moment (μ_g), indicating the excited state of the dye under study is more polar than the ground state and the same trend is noticed with theoretical calculations performed using the CAM‐B3LYP/6‐311+G(d,p) method. Further, the study on preferential solvation was carried out for 3‐MAB dye in ethyl acetate–methanol solvent mixture. The fluorescence quenching method has been employed for the detection of dopamine using 3‐MAB as fluorescent probe, using steady‐state and time resolved methods at room temperature. The method enables dopamine in the micro molar range to be detected. Also, an attempt to verify the quenching process by employing different models has been tried. Various rate parameters are measured using these models, our results indicates the quenching process is diffusion limited.     

Primary steps of the photochemical reactions of 2-cyano-10-(3-[dimethylamino, N-oxide]-2-methylpropyl)-5-oxide-phenothiazine, the photoproduct of cyamemazine, a phototoxic neuroleptic: comparison with the sulfoxide.

The UVA-absorbing photoproduct resulting from the oxidation of the sulfur atom and of the side chain nitrogen of the phototoxic drug cyamemazine (CMZ) (2-cyano-10-(3-[dimethylamino]-2 methylpropyl)-phenothiazine) is a potent photodynamic photosensitizer. The photophysical and photochemical properties of this photoproduct (P) (2-cyano-10-(3-[dimethylamino, N-oxide]-2-methylpropyl)-5-oxide-phenothiazine)) have been investigated in neutral buffered aqueous solutions and in ethanol and compared to those of the sulfoxide (S) (2-cyano-10-(3-[dimethylamino]-2 methylpropyl)-5-oxide-phenothiazine), a CMZ oxidation product of cells. The fluorescence quantum yield (PhiF) of P is 0.25 and 0.21 in pH 7 phosphate buffer and ethanol, respectively. By contrast, S (PhiF = 0.14 in buffer) is practically unfluorescent in alcohol. In buffer, the fluorescence lifetimes of P and S are 10.5 and 11.8 ns, respectively. The transient absorbance of the first excited triplet state (3P1) with a characteristic absorption band peaking at 660 nm (epsilon = 5,300 M(-1) cm(-1)) has been observed by 355 nm laser flash spectroscopy of deaerated phosphate buffer or ethanol solutions. In buffer, the 3P1 lifetime is 0.5 micros. The energy transfer which occurs from the 3P1 to naproxen suggests that the 3P1 energy is greater than 62 kcal mol(-1). Triplet quenching by dioxygen occurs at rate 2.3 x 10(9) M(-1) s(-1). With the triplet benzophenone as actinometer, the 3P1 formation quantum yield is found to be 0. 40 in buffer. The 3P1 state is quenched by ethanol and 2-propanol with bimolecular reaction rate constants of 1.6 and 2.4 x 10(6) M(-1) s(-1), respectively. In buffer, P and S triplet states react with tryptophan, indole and cysteine at rate constants of the order of 10(9) M(-1) s(-1) for Trp and indole and 10(8) M(-1) s(-1) for Cys.     

2-Aminopurine electronic structure and fluorescence properties in DNA

2-Aminopurine (2AP) fluorescence intensity and decay lifetimes have been used as indicators of nucleic acid geometry and dynamics. To characterize 2AP photophysics in the context of a DNA strand, time-dependent density functional theory is applied to 2AP stacked with two flanking nucleobases. Calculations show that 2AP in the trimers suffers a reduction in the oscillator strength of its low-lying pi-pi* 2AP-like allowed transition, manifested in a reduction of its radiative rate. Trimers also exhibit two or three lower-energy excited states (charge transfer states) that are predicted to facilitate nonradiative transitions from the fluorescent excited state.     

Rates of deactivation processes of indole derivatives in water-organic solvent mixtures--application to tryptophyl fluorescence of proteins.

The fluorescence quantum yield and the fluorescence decay of indole, 3-methylindole, 1-methylindole and N-acetyltryptophanamide have been measured in different water-dioxane mixtures. For the first three derivatives, the fluorescence decays were found independent of the emission wavelength and were analyzed as single exponential functions. In the case of N-methylindole the rate of the non radiative deactivation processes knr increased linearly with the molar fraction of dioxane whereas for indole and scatole the variation of knr was biphasic. This behaviour can be explained by two excited state deactivations of these non N-methylated compounds in water and high water content mixtures; one of these deactivation processes occuring through an hydrogen bond between the N-H group and a water molecule. The rate of non radiative deactivation of N-acetyltryptophanamide was dominated by the internal quenching involving the intramolecular carbonyl. The rate of the radiative deactivation process kF of these four compounds increased linearly with the wavenumber of the fluorescence spectrum maximum. Data relative to the three non N-methylated derivatives fell practically on the same straight line. Data from other works have been gathered in order to check if a similar relation between the intrinsic kF and vF values can exist for the tryptophyl fluorescence emission of proteins.     

A series of iridium complexes equipped with inert shields: Highly efficient bluish green emitters with reduced self-quenching effect in solid state

In this paper, we synthesize a series of cyclometalated ligands and their corresponding Ir(III) complexes using pentane-2,4-dione as the auxiliary ligand. We discuss the photophysical properties of these Ir(III) complexes in detail, including their UV-Vis absorption spectra, photoluminescence spectra in solid and liquid states, luminescence decay lifetimes, and luminescence quantum yields. The correlation between self-quenching effect and molecular structure is also investigated. It is found that these Ir(III) complexes are solid-emitting ones due to their reduced self-quenching in solid state. Theoretical calculation and experimental data reveal that the following two reasons should be responsible for the reduced self-quenching in solid state: (1) pentane-2,4-dione, phenyl, and triphenylamine moieties serve as inert shields for the excited state Ir(III) complexes; (2) the radiative decay process in these Ir(III) complexes is accelerated by the introduction of electron-donors, and thus partly immune from self-quenching caused by intermolecular action.     

Photocycle of the flavin-binding photoreceptor AppA, a bacterial transcriptional antirepressor of photosynthesis genes

The flavoprotein AppA from Rhodobacter sphaeroides contains an N-terminal domain belonging to a new class of photoreceptors designated BLUF domains. AppA was shown to control photosynthesis gene expression in response to blue light and oxygen tension. We have investigated the photocycle of the AppA BLUF domain by ultrafast fluorescence, femtosecond transient absorption, and nanosecond flash-photolysis spectroscopy. Time-resolved fluorescence experiments revealed four components of flavin adenine dinucleotide (FAD) excited-state decay, with lifetimes of 25 ps, 150 ps, 670 ps, and 3.8 ns. Ultrafast transient absorption spectroscopy revealed rapid internal conversion and vibrational cooling processes on excited FAD with time constants of 250 fs and 1.2 ps, and a multiexponential decay with effective time constants of 90 ps, 590 ps, and 2.7 ns. Concomitant with the decay of excited FAD, the rise of a species with a narrow absorption difference band near 495 nm was detected which spectrally resembles the long-living signaling state of AppA. Consistent with these results, the nanosecond flash-photolysis measurements indicated that formation of the signaling state was complete within the time resolution of 10 ns. No further changes were detected up to 15 micros. The quantum yield of the signaling-state formation was determined to be 24%. Thus, the signaling state of the AppA BLUF domain is formed on the ultrafast time scale directly from the FAD singlet excited state, without any apparent intermediate, and remains stable over 12 decades of time. In parallel with the signaling state, the FAD triplet state is formed from the FAD singlet excited state at 9% efficiency as a side reaction of the AppA photocycle.     

Molecular mobility and dynamic site heterogeneity in amorphous lactose and lactitol from erythrosin B phosphorescence

We have used phosphorescence from erythrosin B to characterize the molecular mobility and dynamic heterogeneity in dry films of amorphous lactose and lactitol from -25 to 120 degrees C. The phosphorescence emission spectra red-shifted and broadened with temperature in both sugars, indicating that both the rate of dipolar relaxation and the extent of inhomogeneous broadening increased dramatically at higher temperature. Phosphorescence intensity decays were well fit using a stretched exponential decay model; the rate constant for non-radiative quenching due to collisions with the matrix was calculated from the lifetimes. Arrhenius plots of this rate were non-linear, increasing very gradually at low and dramatically at high temperatures in both sugars. The rate of quenching was significantly lower in a 1:1 (wt/wt) mixture of lactose/lactitol in both the glass and the melt, providing strong evidence that specific interactions within the mixture lowered the matrix mobility. The lifetimes varied systematically with emission wavelength in both matrixes; analysis of the temperature dependence indicated that the activation energy for non-radiative quenching of the triplet state varied somewhat with emission wavelength. Time-resolved emission spectra collected as a function of delay time following pulsed excitation exhibited significant shifts to higher energy as a function of time. These data support a photophysical model in which erythrosin B molecules are distributed among matrix sites that vary such that blue-emitting sites with slower rates of matrix dipolar relaxation also have slower rates of molecular collisions. The amorphous matrixes of lactose and lactitol in both the glass and the melt state are thus characterized by dynamic site heterogeneity in which different sites vary in terms of their overall molecular mobility.     

Photophysics of tryptophan in bacteriophage T4 lysozymes

Bacteriophage T4 lysozyme contains three tryptophan residues in distinct environments. Lysozymes with one or two of these residues replaced by tyrosine are used to characterize the photophysics of tryptophan in these individual sites. The fluorescence spectra, average lifetimes, and quantum yields of these three single-tryptophan variants are understandable in terms of the neighboring residues. The emission spectra and radiative lifetimes are found to be the same for all three species while the quantum yield and decay kinetics are quite distinct. The variation of the average nonradiative rate constant is correlated with neighboring quenching groups. Quenching by I- correlates with exposure of the tryptophan residue based on the crystal structure. Complex behavior is observed for the time dependence of the fluorescence decay in all three cases, including that of the immobile tryptophan-138 residue. The complexity of the fluorescence decay is ascribed to heterogeneity in the nonradiative rate constant among microstates. Energy transfer between tryptophan residues is inferred to occur from comparison of the quantum yields of the two-tryptophan and single-tryptophan proteins and is discussed in terms of the F?rster mechanism.     

Temperature effect on the luminescence of synthetized Yt base in PVA film

The mean phosphorescence lifetimes, fluorescence yields and phosphorescence-to-fluorescence quantum yields ratios of Y_t base in PVA films were measured in the temperature range of 100–250°K. The quantum yield of triplet state formation was found to be temperature independent at a wide range of lower temperatures. The radiative and nonradiative rate constants for triplet state were measured.     

Photoluminescence Quenching in Quantum Emitter,Metallic Nanoparticle,and Graphene Hybrids

We have developed a theory for photoluminescence quenching and plasmonic properties in hybrid nanosystems made from three nanosystems such as a quantum emitters, metallic nanoparticles, and graphene. The metallic nanoparticles and graphene have surface plasmons which couple with probe photons and create surface plasmon polaritons. Therefore, the excitons in the quantum emitters interact with surface plasmon polaritons via the dipole-dipole interaction. Due to this interaction, energy is exchanged between the nanosystems. The second quantized formulation and the quantum density matrix method have been used to calculate photoluminescence and the radiative and non-radiative decay processes in the presence of dipole-dipole interaction. We have compared our theory with experiments of two and three nanosystems, and a good agreement between theory and experiments is achieved. It has been found that the photoluminescence quenching in hybrid systems not only occurs through the direct non-radiative energy transfer from the quantum emitter to the metal nanoparticle and to graphene but also occurs through the indirect non-radiative energy transfer from quantum emitter to the metal nanoparticle via graphene and from the quantum emitter to graphene via metal nanoparticle. These are interesting findings and they can be used to fabricate nanoswitches and nanosensors for medical applications.     

Early intermediates in the photocycle of the Glu46Gln mutant of photoactive yellow protein: femtosecond spectroscopy

Transient absorption spectroscopy in the time range from -1 ps to 4 ns, and over the wavelength range from 420 to 550 nm, was applied to the Glu46Gln mutant of the photoactive yellow protein (PYP) from Ectothiorhodospira halophila. This has allowed us to elucidate the kinetic constants of excited state formation and decay and photochemical product formation, and the spectral characteristics of stimulated emission and the early photocycle intermediates. Both the quantum efficiency ( approximately 0.5) and the rate constants for excited state decay and the formation of the initial photochemical intermediate (I(0)) were found to be quite similar to those obtained for wild-type PYP. In contrast, the rate constants for the formation of the subsequent photocycle intermediates (I(0)(double dagger) and I(1)), as well as for I(2) and for ground state regeneration as determined in earlier studies, were found to be from 3- to 30-fold larger. The structural implications of these results are discussed.     

Intramolecular and intermolecular hydrogen-bonding effects on photophysical properties of 2'-aminoacetophenone and its derivatives in solution.

Effects of intra- and intermolecular hydrogen-bonds on the photophysical properties of 2'-aminoacetophenone derivatives (X-C6H4-COCH3) having a substituted amino group (X) with different hydrogen-bonding ability to the carbonyl oxygen (X: NH2(AAP), NHCH3(MAAP), N(CH3)2(DMAAP), NHCOCH3(AAAP), NHCOCF3(TFAAP)) are investigated by means of steady-state and time-resolved fluorescence spectroscopy and time-resolved thermal lensing. Based on the photophysical parameters obtained in aprotic solvents with different polarity and protic solvents with different hydrogen-bonding ability, the characteristic photophysical behavior of the 2'-aminoacetophenone derivatives is discussed in terms of hydrogen-bonding and n,pi*-pi,pi* vibronic coupling. The dominant deactivation process of AAP and MAAP in nonpolar aprotic solvents is the extremely fast internal conversion (k(ic)= 1.0 x 10(11) s(-1) for AAP and 3.9 x 10(10) s(-1) for MAAP in n-hexane). The internal conversion rates of both compounds decrease markedly with increasing solvent polarity, suggesting that vibronic interactions between close-lying S1(pi,pi*) and S2(n,pi*) states lead to the large increase in the non-radiative decay rate of the lowest excited singlet state. It is also suggested that for MAAP, which has a stronger hydrogen-bond as compared to AAP, an intramolecular hydrogen-bonding induced deactivation is involved in the dissipation of the S1 state. For DMAAP, which cannot possess an intramolecular hydrogen-bond, the primary relaxation mechanism of the S1 state in nonpolar aprotic solvents is the intersystem crossing to the triplet state, whereas in protic solvents very efficient internal conversion due to intermolecular hydrogen-bonding is induced. In contrast, the fluorescence spectra of AAAP and TFAAP, which have an amino group with a much stronger hydrogen-bonding ability, give strongly Stokes-shifted fluorescence, indicating that these compounds undergo excited-state intramolecular proton transfer reaction upon electronic excitation.     

Fluorescence Lifetime Imaging of Molecular Rotors in Living Cells

Diffusion is often an important rate-determining step in chemical reactions or biological processes and plays a role in a wide range of intracellular events. Viscosity is one of the key parameters affecting the diffusion of molecules and proteins, and changes in viscosity have been linked to disease and malfunction at the cellular level.^1-3 While methods to measure the bulk viscosity are well developed, imaging microviscosity remains a challenge. Viscosity maps of microscopic objects, such as single cells, have until recently been hard to obtain. Mapping viscosity with fluorescence techniques is advantageous because, similar to other optical techniques, it is minimally invasive, non-destructive and can be applied to living cells and tissues.Fluorescent molecular rotors exhibit fluorescence lifetimes and quantum yields which are a function of the viscosity of their microenvironment.^4,5 Intramolecular twisting or rotation leads to non-radiative decay from the excited state back to the ground state. A viscous environment slows this rotation or twisting, restricting access to this non-radiative decay pathway. This leads to an increase in the fluorescence quantum yield and the fluorescence lifetime. Fluorescence Lifetime Imaging (FLIM) of modified hydrophobic BODIPY dyes that act as fluorescent molecular rotors show that the fluorescence lifetime of these probes is a function of the microviscosity of their environment.^6-8 A logarithmic plot of the fluorescence lifetime versus the solvent viscosity yields a straight line that obeys the Förster Hoffman equation.⁹ This plot also serves as a calibration graph to convert fluorescence lifetime into viscosity.Following incubation of living cells with the modified BODIPY fluorescent molecular rotor, a punctate dye distribution is observed in the fluorescence images. The viscosity value obtained in the puncta in live cells is around 100 times higher than that of water and of cellular cytoplasm.^6,7 Time-resolved fluorescence anisotropy measurements yield rotational correlation times in agreement with these large microviscosity values. Mapping the fluorescence lifetime is independent of the fluorescence intensity, and thus allows the separation of probe concentration and viscosity effects. In summary, we have developed a practical and versatile approach to map the microviscosity in cells based on FLIM of fluorescent molecular rotors.