Polarity of lipid bilayers. A fluorescence investigation.

Through steady-state and time-resolved fluorescence experiments, the polarity of the bilayers of egg phosphatidylcholine vesicles was studied by means of the solvatochromic 2-anthroyl fluorophore which we have recently introduced for investigating the environmental micropolarity of membranes and which was incorporated synthetically in phosphatidylcholine molecules (anthroyl-PC) in the form of 8-(2-anthroyl)octanoic acid. Fluorescence quenching experiments carried out with N,N-dimethylaniline and 12-doxylstearic acid as quenchers showed that the 2-anthroyl chromophore was located in depth in the hydrophobic region of the lipid bilayer corresponding to the C9-C16 segment of the acyl chains. Steady-state fluorescence spectroscopy revealed a nonstructured and red-shifted (lambda em(max) = 464 nm) spectrum for the probe in egg-PC bilayers, which greatly differed from the structured and blue (lambda em(max) = 404 nm) spectrum the fluorophore was shown to display in n-hexane. While the fluorescence decays of the fluorophore in organic solvents were monoexponential, three exponentials were required to account for the fluorescence decays of anthroyl-PC in egg-PC vesicles, with average characteristic times of 1.5 ns, 5.5 ns, and 20 ns. These lifetime values were independent of the emission wavelength used. Addition of cholesterol to the lipid did not alter these tau values. One just observed an increase in the fractional population of the 1.5-ns short-living species detrimental to the population of the 20-ns long-living ones. These observations enabled time-resolved fluorescence spectroscopy measurements to be achieved in the case of the 1/1 (mol/mol) egg-PC/cholesterol mixture. Three distinct decay associated spectra (DAS) were recorded, with maximum emission wavelengths, respectively, of 410 nm, 440 nm, and 477 nm for the 1.5-ns, 6-ns, and 20-ns lifetimes found in this system. On account of the properties and the polarity scale previously established for the 2-anthroyl chromophore in organic solvents, these data strongly suggest the occurrence of three distinct excited states for anthroyl-PC in egg-PC bilayers, corresponding to three environments for the 2-anthroyl chromophore, differing in polarity. The lifetime of 1.5 ns and the corresponding structured and blue (lambda em(max) = 410 nm) DAS account for a hydrophobic environment, with an apparent dielectric constant of 2, which is that expected for the hydrophobic core of the lipid bilayer.(ABSTRACT TRUNCATED AT 400 WORDS)     

The use of n-(9-anthroyloxy) fatty acids to determine fluidity and polarity gradients in phospholipid bilayers

A set of n-(9-anthroyloxy) fatty acid probes (n = 2, 6, 9, 12) have been used to examine gradients in fluorescence polarization, lifetime (tau F), relative quantum yield (phi rel) and positions of emission maxima (lambda max) through bilayers composed of synthetic phospholipids. The fluorophores of these probes report the environment at a graded series of depths from the surface to the centre of the bilayer structure. 1. Polarizations decrease as the fluorophore is moved deeper into the bilayer indicating greater rotational motion of the fluorophore in the hydrocarbon core of the bilayer. 2. The different responses of the probe diphenylhexatriene and the anthroyloxy fatty acids to the action of cholesterol on lipid bilayers are discussed in terms of the orientation of these probes in the bilayer and the types of anisotropic rotational motions which result in depolarization of fluorescence. 3. Stearic acid derivatives which have the fluorophore in the 6-, 9- and 12-positions along the acyl chain have a similar response to solvent polarity as measured by values of lambda max and phi rel in a variety of organic solvents. 4. The position of the emission maximum has little dependence on solvent viscosity, but viscosity does change the degree of vibrational structure seen in the emission spectrum. The vibrational structure itself may be used as an indication of the 'mciroviscosity' gradient in the transverse plane of the bilayer. 5. Values of lambda max, tau F and phi rel indicate that a gradient of polarity exists from the surface to the centre of the bilayer. For dipalmitoyl phosphatidylcholine in the crystalline phase, cholesterol acts to make this polarity gradient shallower.     

Time-resolved fluorescence studies of dityrosine in the outer layer of intact yeast ascospores.

The (time-resolved) fluorescence properties of dityrosine in the outermost layer of the spore wall of Saccharomyces cerevisiae were investigated. Steady-state spectra revealed an emission maximum at 404 nm and a corresponding excitation maximum at 326 nm. The relative fluorescence quantum yield decreased with increasing proton concentration. The fluorescence decay of yeast spores was found to be nonexponential and differed pronouncedly from that of unbound dityrosine in water. Analysis of the spore decay recorded at lambda ex = 323 nm and lambda em = 404 nm by an exponential series (ESM) algorithm revealed a bimodal lifetime distribution with maxima centered at tau 1C = 0.5 ns and tau 2C = 2.6 ns. The relative amplitudes of the two distributions are shown to depend on the emission wavelength, indicating contributions from spectrally different dityrosine chromophores. On quenching the spore fluorescence with acrylamide, a downward curvature of the Stern-Volmer plot was obtained. A multitude of chromophores more or less shielded from solvent in the spore wall is proposed to account for the nonlinear quenching of the total spore fluorescence. Analysis of the fluorescence anisotropy decay revealed two rotational correlation times (phi 1 = 0.9 ns and phi 2 = 30.6 ns) or a bimodal distribution of rotational correlation times (centers at 0.7 ns and 40 ns) when the data were analyzed by the maximum entropy method (MEM). We present a model that accounts for the differences between unbound (aqueous) and bound (incorporated in the spore wall) dityrosine fluorescence. The main feature of the photophysical model for yeast spores is the presence of at least two species of dityrosine chromophores differing in their chemical environments. A hypothetical photobiological role of these fluorophores in the spore wall is discussed: the protection of the spore genome from mutagenic UV light.     

Characterisation of the lowest singlet and triplet excited states of S-flurbiprofen.

The photophysical properties of S-flurbiprofen [S-2-fluoro-alpha-methyl-4-biphenylacetic acid], a nonsteroidal anti-inflammatory drug, have been examined using steady-state and time-resolved spectroscopic techniques. The energy of its first singlet excited state is 99 kcal mol(-1). The fluorescence quantum yields and lifetimes (at 300 nm) have been determined in acetonitrile, methanol, hexane and PBS; they are in the range 0.15相似文献   

Similarity of decay-associated spectra for tryptophan fluorescence of proteins with different structures

Tryptophan fluorescence lifetimes were analyzed for three proteins: human serum albumin, bovine serum albumin, and bacterial luciferase, which contain one, two, and seven tryptophan residues, respectively. For all of the proteins, the fluorescence decays were fitted by three lifetimes: τ₁ = 6–7 ns, τ₂ = 2.0–2.3 ns, and τ₃ ≤ 0.1 ns (the native state), and τ₁ = 4.4–4.6 ns, τ₂ = 1.7–1.8 ns, and τ₃ ≤ 0.1 ns (the denatured state). Corresponding decay-associated spectra had similar peak wavelengths and spectrum half-widths both in the native state (\(\lambda _{\max }^{{\tau _1}} = 324nm\), \(\lambda _{\max }^{{\tau _2}} = 328nm\), and \(\lambda _{\max }^{{\tau _3}} = 315nm\)), and in the denatured state (\(\lambda _{\max }^{{\tau _1}} = 350nm\), \(\lambda _{\max }^{{\tau _2}} = 343nm\), and \(\lambda _{\max }^{{\tau _3}} = 317nm\)). The differences in the steady-state spectra of the studied proteins were accounted for the individual ratio of the lifetime component contributions. The lifetime components were compared with a classification of tryptophan residues in the structure of these proteins within the discrete states model.     

Fluorescence studies of the interaction of DNA with Hoechst 33258

Absorption and fluorescence measurements of DNA-Hoechst 33258 complexes at high molar ratio of DNA phosphate to dye are consistent with the existence of two types of bound species. One type (Type I) predominates at high ionic strength, whereas the other (Type II) occurs at low ionic strength. The fluorescence peak (lambda fmax) depends on the excitation wavelength (lambda ex); lambda fmax shifts toward longer wavelength with increasing lambda ex. Optical properties obtained are summarized in the following: for Type I, lambda amax (absorption) = 352 nm, lambda fmax at lambda ex of 335 nm = 460 nm, tau (fluorescence lifetime) = 2.0-2.5 ns; for Type II, lambda amax = 360 nm, lambda fmax at lambda ex of 335 nm = 470 nm, tau = 4.0-5.0 ns. This behavior is interpreted in terms of solvent-solute relaxation. Type I corresponds to less hydrated bound species, while Type II to more hydrated bound species.     

Solvent effects on fluorescence properties of protochlorophyll and its derivatives with various porphyrin side chains

Fluorescence spectra and fluorescence lifetimes of protochlorophyll (Pchl) were measured in organic solvents having different physical and chemical properties and were analyzed taking into account the nonspecific (dependent on bulk solvent parameters), and specific (e.g. H bonds, Mg coordination) solvent–solute interactions. The energy of the fluorescence emission band decreased, while the Stokes shift increased for increasing solvent orientation polarizability, which is a function of both the dielectric constant (ε) and the refractive index (n). The extent of the dependence of the Stokes shift on solvent orientation polarizability was higher in protic (i.e. those able to form hydrogen-binding) than in aprotic solvents. High value of the Stokes shift was also observed in pyridine and methanol, i.e. in solvents hexacoordinating the central Mg atom. The fluorescence decay of Pchl was monoexponential in all of the investigated solvents. The fluorescence lifetime decreased for increasing solvent orientation polarizability from 5.5 ± 0.1 ns in 1,4-dioxane to 3.3 ± 0.1 ns in methanol. Longer lifetime values were observed in the case of aprotic solvents than in protic solvents. The hexacoordination of Mg had no effect on the fluorescence lifetime. The present data are discussed with respect to results found for protochlorophyllide (Pchlide) (My?liwa-Kurdziel et al. in Photochem Photobiol 79:62–67, 2004), and they indicate that the presence of phytol chain in the porphyrin ring influences the spectral properties of the whole chromophore. This is the first complex analysis comparing the fluorescence emission and fluorescence lifetimes of purified Pchl and Pchlide.     

Dual photoactive species in Glu46Asp and Glu46Ala mutants of photoactive yellow protein: a pH-driven color transition.

Photoactive yellow protein (PYP) is a blue light sensor present in the purple photosynthetic bacterium Ectothiorhodospira halophila, which undergoes a cyclic series of absorbance changes upon illumination at its lambda(max) of 446 nm. The anionic p-hydroxycinnamoyl chromophore of PYP is covalently bound as a thiol ester to Cys69, buried in a hydrophobic pocket, and hydrogen-bonded via its phenolate oxygen to Glu46 and Tyr42. The chromophore becomes protonated in the photobleached state (I(2)) after it undergoes trans-cis isomerization, which results in breaking of the H-bond between Glu46 and the chromophore and partial exposure of the phenolic ring to the solvent. In previous mutagenesis studies of a Glu46Gln mutant, we have shown that a key factor in controlling the color and photocycle kinetics of PYP is this H-bonding system. To further investigate this, we have now characterized Glu46Asp and Glu46Ala mutants. The ground-state absorption spectrum of the Glu46Asp mutant shows a pH-dependent equilibrium (pK = 8.6) between two species: a protonated (acidic) form (lambda(max) = 345 nm), and a slightly blue-shifted deprotonated (basic) form (lambda(max) = 444 nm). Both of these species are photoactive. A similar transition was also observed for the Glu46Ala mutant (pK = 7.9), resulting in two photoactive red-shifted forms: a basic species (lambda(max) = 465 nm) and a protonated species (lambda(max) = 365 nm). We attribute these spectral transitions to protonation/deprotonation of the phenolate oxygen of the chromophore. This is demonstrated by FT Raman spectra. Dark recovery kinetics (return to the unphotolyzed state) were found to vary appreciably between these various photoactive species. These spectral and kinetic properties indicate that the hydrogen bond between Glu46 and the chromophore hydroxyl group is a dominant factor in controlling the pK values of the chromophore and the glutamate carboxyl.     

Intrinsic tryptophan fluorescence identifies specific conformational changes at the actomyosin interface upon actin binding and ADP release.

The helix-loop-helix (A-site) and myopathy loop (R-site) are located on opposite sides of the cleft that separates the proposed actin-binding interface of myosin. To investigate the structural features of the A- and R-sites, we engineered two mutants of the smooth muscle myosin motor domain with the essential light chain (MDE), containing a single tryptophan located either in the A-site (W546-MDE) or in the R-site (V413W MDE). W546- and V413W-MDE display actin-activated ATPase and actin-binding properties similar to those of wild-type MDE. The steady-state fluorescence properties of W546-MDE [emission peak (lambda(max)) = 344, quantum yield = 0.20, and acrylamide bimolecular quenching constant (k(q)) = 6.4 M(-)(1). ns(-)(1)] and V413W-MDE [lambda(max) = 338, quantum yield = 0.27, and k(q) = 3.6 M(-)(1).ns(-)(1)] demonstrate that Trp-546 and Trp-413 are nearly fully exposed to solvent, in agreement with the crystallographic data on these residues. In the presence of actin, Trp-546 shifts to a more buried environment in both the ADP-bound and nucleotide-free (rigor) actomyosin complexes, as indicated by an average lambda(max) of 337 or 336 nm, respectively, and protection from dimethyl(2-hydroxy-5-nitrobenzyl)sulfonium bromide (DHNBS) oxidation. In contrast, Trp-413 has a single conformation with an average lambda(max) of 338 nm in the ADP-bound complex, but in the rigor complex it is 50% more accessible to DHNBS oxidation and can adopt a range of possible conformations (lambda(max) = 341-347 nm). Our results suggest a structural model in which the A-site remains tightly bound to actin and the R-site adopts a more flexible and solvent-exposed conformation upon ADP release.     

Antioxidants as aromatic amino acid oxidation products

The accumulation of UV photolysis products of amino acids tyrosine and tryptophan, which possess an antioxidant activity, has been studied by the method of luminol-activated chemiluminescence. The amount of antioxidant products was judged by the value of the total antioxidant potential of a UV-irradiated solution, the measure of which was the distance between the peaks of the chemiluminescence curve in the system 2,2'-azo-bis(2-amidinopropane)hydrochloride + luminol in a UV-irradiated and an unirradiated samples (induction period, tau(i)). Simultaneously, the absorption and fluorescence spectra of unirradiared and UV-irradiated amino acid solutions were recorded. It was shown that, upon the exposure of a tryptophan solution to radiation, the accumulation of the fluorescent product N-formyl kynurenine (lambda(em) = 325 nm, lambda(max) = 440 nm) occures, and the curve of its accumulation was similar to the curve of growth of tau(i) photoproducts produced during UV-radiation. When a tyrosine solution was irradiated, the main fluorescent product was dityrosine (lambda(em) = 310 nm, lambda(max) = 415 nm). Nevertheless, the dose dependencies of the formation of dityrosine, and the total antioxidant potential (tau(i)) were completely different. It was found that another product of tyrosine UV-photolysis, dioxyphenylalanine, possessed a pronounced antioxidant activity. It was concluded that the main antioxidants produced under UV-irradiation of tryptophan is formyl kynurenine, and under the irradiation of tyrosine, dioxyphenylalanine.     

Fluorescence studies of phosphoribulokinase, a light-regulated, chloroplastic enzyme

Recent characterization of spinach phosphoribulokinase has revealed that the homodimeric molecule contains only two tryptophans per 44-kDa subunit. We have performed steady-state and frequency domain studies of the intrinsic fluorescence of this protein. The fluorescence properties reflect contributions from both types of tryptophan residues. One of these appears to be relatively exposed to solvent and the quencher, acrylamide; fluoresce with a lambda max of 345 nm; decay with a fluorescence lifetime of 6.3 ns; have a relatively red-shifted absorption spectrum; and have a certain degree of independent motional freedom, with respect to the protein. The other tryptophan residue appears to be more buried; fluoresce with lambda max of 325 nm; have a lifetime of 1.7 ns; have a relatively blue-shifted absorption spectrum; and not to enjoy independent motional freedom. On comparison of phase-resolved spectral data and solute quenching data, we suggest that resonance energy transfer between the blue and red tryptophan residues may occur. We also describe the strategy of simultaneously fitting Stern-Volmer quenching data collected at two emission wavelengths.     

Purification of the yellow fluorescent protein from Vibrio fischeri and identity of the flavin chromophore

A low molecular weight protein (approximately 25,000 D) exhibiting a yellow fluorescence emission peaking at approximately 540 nm was isolated from Vibrio fischeri (strain Y-1) and purified to apparent homogeneity. FMN is the chromophore, but it exhibits marked red shifts in both the absorption (lambda max = 380, 460 nm) and the fluorescence emission. When added to purified luciferase from the same strain, which itself catalyzes an emission of blue-green light (lambda max approximately 495 nm), this protein induces a bright yellow luminescence (lambda max approximately 540 nm); this corresponds to the emission of the Y-1 strain in vivo. This yellow bioluminescence emission is thus ascribed to the interaction of these two proteins, and to the excitation of the singlet FMN bound to this fluorescent protein.     

Protein-flavonol interaction: fluorescence spectroscopic study

Recent studies have shown that various synthetic as well as therapeutically active naturally occurring flavonols possess novel luminescence properties that can potentially serve as highly sensitive monitors of their microenvironments in biologically relevant systems. We report a study on the interactions of bovine serum albumin (BSA) with the model flavonol 3-hydroxyflavone (3HF), using the excited-state proton-transfer (ESPT) luminescence of 3HF as a probe. Upon addition of BSA to the flavonoid solutions, we observe remarkable changes in the absorption, ESPT fluorescence emission and excitation profiles as well as anisotropy (r) values. Complexation of 3HF with protein results in a pronounced shift (20 nm) of the ESPT emission maximum of the probe (from lambda(max)(em) = 513 nm to lambda(max)(em) = 533 nm) accompanied by a significant increase in fluorescence intensity. The spectral data also suggest that, in addition to ESPT, the protein environment induces proton abstraction from 3HF leading to formation of anionic species in the ground state. Fairly high values of anisotropy are observed in the presence of BSA for the tautomer (r = 0.25) as well as anion (r = 0.35) species of 3HF, implying that both the species are located in motion-restricted environments of BSA molecules. Analysis of relevant spectroscopic data leads to the conclusions that two binding sites are involved in BSA-3HF interaction, and the interaction is slightly positively cooperative in nature with a similar binding constant of 1.1 - 1.3 x 10(5) M(-1) for both these sites. Proteins 2001;43:75-81.     

Long-lived fluorescence lifetime from tyrosine in a peptide derived from S-100b.

It was shown in an earlier report (Turner et al., 1989, Biochem. Cell Biol. 67; 179-186) that the anomalous steady-state fluorescence emission spectra observed for the protein S-100b in aqueous solution at pH 7.5 contains a long-lived fluorescence decay component. In this study, a peptide consisting of residues 11 to 27 of the beta-subunit, was investigated. 11Ile-Asp-Val-Phe-His15-Gln-Tyr-Ser-Gly-Arg20-Glu-Gly- Asp-Lys-His25-Lys-Leu27 Fluorescence lifetimes were measured at the emission maximum and in the red edge of the spectrum. At wavelengths greater than 320 nm, the data was best fit with three exponentials. The third exponential gave lifetimes of 13.1 ns and 15.9 ns when the peptide was dissolved in the solvents propane-2-ol and propane-1,2-diol, respectively (lambda EX = 275 nm, lambda EM = 350 nm). These fluorescence lifetimes are similar to that observed for a decay component of native S-100b in the red edge of the emission, suggesting that the 1 degrees and 2 degrees features of a heptadecapeptide from S-100b protein has enough structural information when dissolved in solvents of intermediate polarity provide appropriate conditions for long-lived fluorescence from a tyrosine/tyrosinate species to occur.     

Spatial relationship between a fast-reacting thiol and a reactive lysine residue of myosin subfragment 1

Fluorescence energy transfer was used to examine the spatial proximity between two key side chains in myosin subfragment 1 (S-1), viz., the reactive thiol (SH1) located on the C-terminal 20K tryptic fragment and the reactive lysyl (RLR) on the N-terminal 27K tryptic fragment of S-1 heavy chain. S-1 was specifically labeled at SH1 with an energy donor, N-(iodoacetyl)-N'-(5-sulfo-1-naphthyl)ethylenediamine (AEDANS), and at RLR with an energy acceptor, 2,4,6,-trinitrobenzenesulfonate (TNBS). Prior blocking of SH1 with AEDANS increased the pK of RLR from 9.04 to 9.42. Trinitrophenylation of SH1-blocked S-1 was about 50% slower and sharply reduced the Ca2+ ATPase activity. Reciprocally, blocking of RLR with TNBS slowed the rate of reaction of SH1 and AEDANS by 40-60%. Addition of the second label does not grossly alter the conformation resulting from the first label. S-1 labeled at RLR with TNBS and at SH1 with optically inert iodoacetamide shows the same TNP difference spectrum +/- MgADP (lambda min 365 nm) as S-1 with S 1 free. Also, S-1 labeled at SH1 with AEDANS and at RLR with an optically inert methyl group shows the same AEDANS emission spectrum (lambda em max 475 nm), excited-state lifetime (tau = 20.3 ns) and rotational correlation time (phi = 106 ns) as S-1 with RLR free. When the decrease of either the quantum yield or the excited-state lifetime of the donor in the absence and presence of the acceptor was measured, the energy transfer efficiency was found to be 70%. The apparent interchromophore distance was calculated to be 2.6 nm through the use of the F?rster equation with an uncertainty of less than 12%.     

Bioluminescence spectral and fluorescence dynamics study of the interaction of lumazine protein with the intermediates of bacterial luciferase bioluminescence

The mechanism of the shifting of the bioluminescence spectrum from the reaction of bacterial luciferase by lumazine protein is investigated by methods of fluorescence dynamics. A metastable intermediate is produced on reaction of Vibrio harveyi luciferase with FMNH2 and O2. It has an absorption maximum at 374 nm and a rotational correlation time (phi) derived from the decay of its fluorescence (maximum 500 nm) anisotropy of 90 ns (2 degrees C). Lumazine protein from Photobacterium phosphoreum has an absorption maximum at 417 nm and a fluorescence maximum at 475 nm. Lumazine protein forms a protein-protein complex with luciferase, and the complex has a phi of approximately 100 ns. A mixture of lumazine protein and the intermediate would be expected to have an average correlation time (phi av) around 100 ns, but instead, the result is anomalous. The phi av is much lower and is also wavelength dependent. For excitation at 375 nm, which is mainly absorbed in the flavin chromophore of the intermediate, phi av = 25 ns, but at 415 nm, mainly absorbed by the lumazine derivative ligand of lumazine protein, phi av approximately 50 ns. It is proposed that protein-protein complexation occurs between lumazine protein and the luciferase intermediate and that in this complex energy transfer from the flavin to the lumazine is the predominant channel of anisotropy loss. A distance of 20 A between the donor and acceptor is calculated. In the bioluminescence reaction of intermediate with tetradecanal, a fluorescent transient species is produced which is the bioluminescence emitter.(ABSTRACT TRUNCATED AT 250 WORDS)     

Polarized absorption spectra of green fluorescent protein single crystals: transition dipole moment directions

Polarized absorption spectra of orthorhombic crystals of wild-type green fluorescent protein (GFP) were measured between 350 and 520 nm to obtain information on the directions of the electronic transition dipole moments ((-->)m) of the chromophore relative to the molecular axes. The transition dipole moment orientation is a basic spectroscopic parameter of relevance to biologists when interpreting F?rster-type fluorescence resonance energy transfer data and for comparing absorbance and fluorescence spectra of GFP with quantum chemical calculations. Maximal extinction was obtained throughout the spectrum when the polarization direction of the electric vector of incident light was parallel to the c-axis of the crystal. The transition dipole moments were assumed to be parallel to the plane of the chromophore. With this assumption and the measured dichroic ratios in the crystals, the transition dipole moments associated with the neutral (lambda(max) = 398 nm) and anionic (lambda(max) = 478 nm) forms of the chromophore were found to subtend angles of approximately 26 degrees and 13 degrees (counterclockwise), respectively, with the vector that joins the phenolic and imidazolinone oxygen atoms of the chromophore.     

Action mechanism of Escherichia coli DNA photolyase. III. Photolysis of the enzyme-substrate complex and the absolute action spectrum

The absolute action spectrum of Escherichia coli DNA photolyase was determined in vitro. In vivo the photoreactivation cross-section (epsilon phi) is 2.4 X 10(4) M-1 cm-1 suggesting that the quantum yield (phi) is about 1.0 if one assumes that the enzyme has the same spectral properties (e.g. epsilon 384 = 1.8 X 10(4) M-1 cm-1) in vivo as those of the enzyme purified to homogeneity. The relative action spectrum of the pure enzyme (blue enzyme that contains FAD neutral semiquinone radical) agrees with the relative action spectrum for photoreactivation of E. coli, having lambda max = 384 nm. However, the absolute action spectrum of the blue enzyme yields a photoreactivation cross-section (epsilon phi = 1.2 X 10(3) at 384 nm) that is 20-fold lower than the in vivo values indicative of an apparent lower quantum yield (phi approximately equal to 0.07) in vitro. Reducing the enzyme with dithionite results in reduction of the flavin semiquinone and a concomitant 12-15-fold increase in the quantum yield. These results suggest that the flavin cofactor of the enzyme is fully reduced in vivo and that, upon absorption of a single photon in the 300-500 nm range, the photolyase chromophore (which consists of reduced FAD plus the second chromophore) donates an electron to the pyrimidine dimer causing its reversal to two pyrimidines. The reduced chromophore is regenerated at the end of the photochemical step thus enabling the enzyme to act catalytically.+     

Photophysical behaviour of 1-(4-N,N-dimethylaminophenylethynyl)pyrene (DMAPEPy) in homogeneous media.

The photophysical behaviour of a new pyrene derivative, 1-(4-N,N-dimethylaminophenylethynyl)pyrene (DMAPEPy), in various solvents has been studied. Due to the presence of an ethynyl link with a cylindrical pi cloud between the donor (N,N-dimethyl group) and the acceptor (pyrene), the molecule shows efficient intramolecular charge transfer, with a high extinction coefficient in all the solvents. There is significant solvatochromism in the fluorescence with a large increase in the Stokes' shift of around 125 nm between n-hexane and acetonitrile. The solvent-dependent spectral data show a good correlation with the Kamlet-Taft solvent polarity parameter (pi*). The plots of Stokes' shifts with E(T)(30) are linear for non-protic solvents and for protic solvents but with different slopes. The fluorescence quantum yields are high for non-polar solvents and decrease as the solvent polarity increases. Unlike the parent molecule pyrene, DMAPEPy shows a short lifetime, which is fairly insensitive to oxygen-induced quenching and is dependent on solvent polarity. The molecule shows high steady-state fluorescence anisotropy, which is very sensitive to the viscosity change of the medium.     

Kindling fluorescent protein from Anemonia sulcata: dark-state structure at 1.38 A resolution

When the nonfluorescent chromoprotein asFP595 from Anemonia sulcata is subjected to sufficiently intense illumination near the absorbance maximum (lambda(abs)(max) = 568 nm), it undergoes a remarkable transition, termed "kindling", to a long-lived fluorescent state (lambda(em)(max) = 595 nm). In the dark recovery phase, the kindled state relaxes thermally on a time scale of seconds or can instantly be reverted upon illumination at 450 nm. The kindling phenomenon is enhanced by the Ala143 --> Gly point mutation, which slows the dark recovery time constant to 100 s at room temperature and increases the fluorescence quantum yield. To investigate the chemical nature of the chromophore and the possible role of chromophore isomerization in the kindling phenomenon, we determined the crystal structure of the "kindling fluorescent protein" asFP595-A143G (KFP) in the dark-adapted state at 1.38 A resolution and 100 K. The chromophore, derived from the Met63-Tyr64-Gly65 tripeptide, closely resembles that of the nonfluorescent chromoprotein Rtms5 in that the configuration is trans about the methylene bridge and there is substantial distortion from planarity. Unlike in Rtms5, in the native protein the polypeptide backbone is cleaved between Cys62 and Met63. The size and shape of the chromophore pocket suggest that the cis isomer of the chromophore could also be accommodated. Within the pocket, partially disordered His197 displays two conformations, which may constitute a binary switch that stabilizes different chromophore configurations. The energy barrier for thermal relaxation was found by Arrhenius plot analysis to be approximately 71 kJ/mol, somewhat higher than the value of approximately 55 kJ/mol observed for cis-trans isomerization of a model chromophore in solution.