Time-resolved fluorescence analysis of the recombinant photosystem II antenna complex CP29. Effects of zeaxanthin, pH and phosphorylation.

Nonradiative dissipation of excitation energy is the major photoprotective mechanism in plants. The formation of zeaxanthin in the antenna of photosystem II has been shown to correlate with the onset of nonphotochemical quenching in vivo. We have used recombinant CP29 protein, over-expressed in Escherichia coli and refolded in vitro with purified pigments, to obtain a protein indistinguishable from the native complex extracted from thylakoids, binding either violaxanthin or zeaxanthin together with lutein. These recombinant proteins and the native CP29 were used to measure steady-state chlorophyll fluorescence emission and fluorescence decay kinetics. We found that the presence of zeaxanthin bound to CP29 induces a approximately 35% decrease in fluorescence yield with respect to the control proteins (the native and zeaxanthin-free reconstituted proteins). Fluorescence decay kinetics showed that four components are always present but lifetimes (tau) as well as relative fluorescence quantum yields (rfqy) of the two long-lived components (tau3 and tau4) are modified by the presence of zeaxanthin. The most relevant changes are observed in the rfqy of tau3 and in the average lifetime ( approximately 2.4 ns with zeaxanthin and 3.2-3.4 ns in the control proteins). When studied in vitro, no significant effect of acidic pH (5.2-5.3) is observed on chlorophyll A fluorescence yield or kinetics. The data presented show that recombinant CP29 is able to bind zeaxanthin and this protein-bound zeaxanthin induces a significant quenching effect.     

Nonequivalent binding sites in cystathionase. Nanosecond and steady fluorescence studies.

The analogs P-pyridoxyl-L-alanine and P-pyridoxyl-L-homoserine bind to the apoprotein of the enzyme cystathionase and inhibit the reactivation of enzymatic activity after addition of pyridoxyl-5-P. The binding of the inhibitors was monitored by measuring the fluorescence emitted by the P-pyridoxyl moiety at 395 nm (excitation 325 nm). The fluorometric titration results indicate the presence of nonequivalent binding sites in the apoprotein. A model based on two classes of independent binding sites fits the fluorometric data reasonably well. The presence of nonequivalent fluorescent sites in reduced cystathionase was also detected by nanosecond spectroscopy. In contrast to the model compound P-pyridoxyl-epsilon-lysine (tau equals 2.6 ns), the P-pyridoxyl residues of cystathionase display multiexponential fluorescence decay. Two fluorescence lifetimes (tau2 equals 4.1 ns and tau2 equals 15 ns) fit the deconvoluted decay results obtained by pulse fluorimetry. It is proposed that the P-pyridoxyl chromophores of reduced cystathionase have different environments.     

Time-resolved fluorescence analysis of the photosystem II antenna proteins in detergent micelles and liposomes

We have studied the time-resolved fluorescence properties of the light-harvesting complexes (Lhc) of photosystem II (Lhcb) in order to obtain information on the mechanism of energy dissipation (non-photochemical quenching) which is correlated to the conversion of violaxanthin to zeaxanthin in excess light conditions. The chlorophyll fluorescence decay of Lhcb proteins LHCII, CP29, CP26, and CP24 in detergent solution is mostly determined by two lifetime components of 1.2-1.5 and 3.6-4 ns while the contribution of the faster component is higher in CP29, CP26, and CP24 with respect to LHCII. The xanthophyll composition of Lhc proteins affects the ratio of the lifetime components: when zeaxanthin is bound into the site L2 of LHCII, the relative amplitude of the faster component is increased and, consequently, the chlorophyll fluorescence quenching is enhanced. Analysis of quenching in mutants of Arabidopsis thaliana, which incorporate either violaxanthin or zeaxanthin in their Lhc proteins, shows that the extent of quenching is enhanced in the presence of zeaxanthin. The origin of the two fluorescence lifetimes was analyzed by their temperature dependence: since lifetime heterogeneity was not affected by cooling to 77 K, it is concluded that each lifetime component corresponds to a distinct conformation of the Lhc proteins. Upon incorporation of Lhc proteins into liposomes, a quenching of chlorophyll fluorescence was observed due to shortening of all their lifetime components: this indicates that the equilibrium between the two conformations of Lhcb proteins is displaced toward the quenched conformation in lipid membranes or thylakoids with respect to detergent solution. By increasing the protein density in the liposomes, and therefore the probability of protein-protein interactions, a further decrease of fluorescence lifetimes takes place down to values typical of quenched leaves. We conclude that at least two major factors determine the quenching of chlorophyll fluorescence in Lhcb proteins, i.e., intrasubunit conformational change and intersubunit interactions within the lipid membranes, and that these processes are both important in the photoprotection mechanism of nonphotochemical quenching in vivo.     

Detection of a pH-dependent conformational change in azurin by time-resolved phosphorescence.

Azurin, a blue copper protein from the bacterial species Pseudomonas aeruginosa, contains a single tryptophan residue. Previous fluorescence measurements indicate that this residue is highly constrained and unusually inaccessible to water. In the apoprotein this residue also possesses a long-lived room-temperature phosphorescence (RTP), the nonexponential decay of which can be resolved into two major components associated with lifetimes of 417 and 592 ms, which likely originate from at least two conformations of the protein. The relative weights of these two decay components change with pH in good correlation with a change in protonation of His-35, which has been studied in Cu(II) azurin. Interestingly, the structural changes characterized in earlier work have little effect on the fluorescence decay and appear to occur away from the tryptophan residue. However, in the present work, the two RTP lifetimes suggest conformations with different structural rigidities in the vicinity of the tryptophan residue. The active conformation that predominates below a pH of 5.6 has the shorter lifetime and is less rigid. Phosphorescence decays of several metal derivatives of azurin were also measured and revealed strong similarities to that of apoazurin, indicating that the structural constraints upon the metal-binding site are imposed predominately by the protein.     

A time-resolved fluorescence study of human copper-zinc superoxide dismutase

The intrinsic fluorescence decay of human Cu,Zn superoxide dismutase was measured by frequency-domain techniques. The protein consists of two subunits, each containing one tryptophan and no tyrosine residues. Using a synchrotron radiation source, which allows facile selection of the excitation wavelength, the dependence of the emission decay upon excitation was studied. No significant excitation wavelength effects were found. The two tryptophans contained in the dimer, although fully equivalent and exposed to solvent, showed a fluorescence decay that cannot be described by a single lifetime. Either two lifetimes, or one Lorentzian-shaped continuous distribution of lifetimes, are needed to obtain a good fit. Under identical experimental conditions, control experiments showed that N-acetyltryptophanamide, an analogue of tryptophanyl residues in proteins, decays with a single lifetime. The heterogeneous decay of tryptophan fluorescence in superoxide dismutase is interpreted as due to the presence of static and/or dynamic conformers in the protein that decay with different lifetimes. The two models of discrete lifetimes and continuous distribution of lifetimes are discussed with reference to measurements on holo- and apo-human superoxide dismutase.     

Antisense inhibition of the photosynthetic antenna proteins CP29 and CP26: implications for the mechanism of protective energy dissipation

The specific roles of the chlorophyll a/b binding proteins CP29 and CP26 in light harvesting and energy dissipation within the photosynthetic apparatus have been investigated. Arabidopsis was transformed with antisense constructs against the genes encoding the CP29 or CP26 apoprotein, which gave rise to several transgenic lines with remarkably low amounts of the antisense target proteins. The decrease in the level of CP24 protein in the CP29 antisense lines indicates a physical interaction between these complexes. Analysis of chlorophyll fluorescence showed that removal of the proteins affected photosystem II function, probably as a result of changes in the organization of the light-harvesting antenna. However, whole plant measurements showed that overall photosynthetic rates were similar to those in the wild type. Both antisense lines were capable of the qE type of nonphotochemical fluorescence quenching, although there were minor changes in the capacity for quenching and in its induction kinetics. High-light-induced violaxanthin deepoxidation to zeaxanthin was not affected, although the pool size of these pigments was decreased slightly. We conclude that CP29 and CP26 are unlikely to be sites for nonphotochemical quenching.     

Identity of the Photosystem II reaction center polypeptide

A Photosystem-II (PS-II)-enriched chloroplast submembrane fraction has been subjected to non-denaturing gel-electrophoresis. Two chlorophyll a (Chl a)-binding proteins associated with the core complex were isolated and spectrally characterized. The Chl protein with apparent apoprotein mass of 47 kDa (CP47) displayed a 695 nm fluorescence emission maximum (77 K) and light-induced absorption characteristics indicating the presence of the reaction center Chl, P-680, and its primary electron acceptor, pheophytin. A Chl protein of apparent apoprotein mass of 43 kDa (CP43) displayed a fluorescence emission maximum at 685 nm. We conclude that CP43 serves as an antenna Chl protein and the PS II reaction center is located in CP47.     

Viscosity Dependence of Primary Photoprocesses of 124 Kilodalton Phytochrome

To characterize the nature of primary photoprocesses of phytochrome which serves as the red-far red reversible photoreceptor for photomorphogenesis in plants, viscosity dependence of the fluorescence lifetimes of phytochrome isolated from etiolated oat seedling (Avena sativa L.) has been investigated. The fluorescence decay of phytochrome exhibited approximately two components, one with lifetime in the range of 50-70 ps and another with 1.1-1.2 ns in phosphate buffer with or without 40-67% glycerol. However, relative amplitudes of these decay components were found to be strongly viscosity dependent. Thus, the longer decay component increased from 2-5% in phosphate buffer to ~20% in 67% glycerol-phosphate buffer. These results have been interpreted in terms of primary reaction from the excited singlet state of phytochrome, yielding a photoreversible intermediate whose rate of formation and decay were apparently viscosity-dependent. Further, the viscosity dependence is consistent with the primary reaction involving conformational changes of the chromophore/its apoprotein environment.     

Energy dissipation efficiency in the CP43 assembly intermediate complex of photosystem II

Photosystem II in oxygenic organisms is a large membrane bound rapidly turning over pigment protein complex. During its biogenesis, multiple assembly intermediates are formed, including the CP43-preassembly complex (pCP43). To understand the energy transfer dynamics in pCP43, we first engineered a His-tagged version of the CP43 in a CP47-less strain of the cyanobacterium Synechocystis 6803. Isolated pCP43 from this engineered strain was subjected to advanced spectroscopic analysis to evaluate its excitation energy dissipation characteristics. These included measurements of steady-state absorption and fluorescence emission spectra for which correlation was tested with Stepanov relation. Comparison of fluorescence excitation and absorptance spectra determined that efficiency of energy transfer from β-carotene to chlorophyll a is 39 %. Time-resolved fluorescence images of pCP43-bound Chl a were recorded on streak camera, and fluorescence decay dynamics were evaluated with global fitting. These demonstrated that the decay kinetics strongly depends on temperature and buffer used to disperse the protein sample and fluorescence decay lifetime was estimated in 3.2–5.7 ns time range, depending on conditions. The pCP43 complex was also investigated with femtosecond and nanosecond time-resolved absorption spectroscopy upon excitation of Chl a and β-carotene to reveal pathways of singlet excitation relaxation/decay, Chl a triplet dynamics and Chl a → β-carotene triplet state sensitization process. The latter demonstrated that Chl a triplet in the pCP43 complex is not efficiently quenched by carotenoids. Finally, detailed kinetic analysis of the rise of the population of β-carotene triplets determined that the time constant of the carotenoid triplet sensitization is 40 ns.     

The effect of thylakoid membrane reorganisation on chlorophyll fluorescence lifetime components: A comparison between state transitions,protein phosphorylation and the absence of Mg2+

Room temperature chlorophyll fluorescence lifetime measurements using single photon counting and low-intensity laser excitation have been carried out on photosynthetic systems which have undergone protein reorganisation by an in vivo state 1-state 2 transition, protein phosphorylation and the absence of Mg²⁺. Analysis of the global changes in average lifetime and total fluorescence yield suggest that each treatment brings about a decrease in Photosystem (PS) II absorption cross-section but that this mechanism of energy redistribution accounts for different proportions of the total fluorescence quenching in the various cases. Further analysis of the overall fluorescence decay into individual kinetic components was carried out using a four-exponential model. The state transition did not alter the lifetimes of the four components but decreased the fluorescence yield of the long-lived decay, at both F₀ and F_M, by 24% and increased the yield of the rapid components. Such changes infer that there is a decrease in PS II absorption cross-section and an increase in PS I excitation on going from state 1 to state 2. Furthermore, these alterations show that the 500 ps component (at F₀) gives rise to the 2 ns decay (at F_M). After in vitro protein phosphorylation at 5 mM Mg²⁺, the changes are very similar to those brought abought by a state transition, except that both long-lived kinetic components exhibit a decrease in yield. When protein phosphorylation was carried out at 2 mM Mg²⁺ a slight decrease in the lifetimes of the two slow components was observed, with a further decrease in the yield of the 2.3 ns decay and a larger increase in the yields of the two rapid decays. Although the fluorescence quenching brought about by the absence of Mg²⁺ (57%) was the largest of all the treatments, only a small part could be explained by a decrease in PS II absorption cross-section (17%). The absence of Mg²⁺ led to a decrease in the lifetimes and yields of the two long-lived decays. A careful comparison of the characteristics of the slowest component in the presence and absence of 5 mM Mg²⁺ on closing the PS II traps suggest that this decay has different origins in the two cases.     

Interpretation of fluorescence decays using a power-like model

A power-like decay function, characterized by the mean excited-state lifetime and relative variance of lifetime fluctuation around the mean value, was applied in analysis of fluorescence decays measured with the aid of time-correlated single photon counting. We have examined the fluorescence decay, in neutral aqueous medium, of tyrosine (L-tyrosine and N-acetyl-L-tyrosinamide), and of the tyrosine residues in a tryptophan-free protein, the enzyme purine nucleoside phosphorylase from Escherichia coli in a complex with formycin A (an inhibitor), and orthophosphate (a co-substrate). Tryptophan fluorescence decay was examined in neutral aqueous medium for L-tryptophan, N-acetyl-L-tryptophanamide, and for two tryptophan residues in horse liver alcohol dehydrogenase. To detect solvent effect, fluorescence decay of Nz-acetyl-L-tryptophanamide in aqueous medium was compared with that in dioxan. Hitherto, complex fluorescence decays have usually been analyzed with the aid of a multiexponential model, but interpretation of the individual exponential terms (i.e., pre-exponential amplitudes and fluorescence lifetimes), has not been adequately characterized. In such cases the intensity decays were also analyzed in terms of the lifetime distribution as a consequence of an interaction of fluorophore with environment. We show that the power-like decay function, which can be directly obtained from the gamma distribution of fluorescence lifetimes, is simpler and provides good fits to highly complex fluorescence decays as well as to a purely single-exponential decay. Possible interpretation of the power-like model is discussed.     

Long-lived primary radical pair state detected by time-resolved fluorescence and absorption spectroscopy in an isolated Photosystem two core

A Photosystem two (PS II) core preparation containing the chlorophyll a binding proteins CP 47, CP 43, D1 and D2, and the non-chlorophyll binding cytochrome-b559 and 33 kDA polypeptides, has been isolated from PS II-enriched membranes of peas using the non-ionic detergent heptylthioglucopyranoside and elevated ionic strengths. The primary radical pair state, P680⁺Pheo^-, was studied by time-resolved absorption and fluorescence spectroscopy, under conditions where quinone reduction and water-splitting activities were inhibited. Charge recombination of the primary radical pair in PS II cores was found to have lifetimes of 17.5 ns measured by fluorescence and 21 ns measured by transient decay kinetics under anaerobic conditions. Transient absorption spectroscopy demonstrated that the activity of the particles, based on primary radical pair formation, was in excess of 70% (depending on the choice of kinetic model), while time-resolved fluorescence spectroscopy indicated that the particles were 91% active. These estimates of activity were further supported by steady-state measurements which quantified the amount of photoreducible pheophytin. It is concluded that the PS II core preparation we have isolated is ideal for studying primary radical pair formation and recombination as demonstrated by the correlation of our absorption and fluorescence transient data, which is the first of its kind to be reported in the literature for isolated PS II core complexes from higher plants.Abbreviations CP 43 and CP 47 chlorophyll binding proteins of PS II having apparent molecular weights on SDS-PAGE of 43 kDa and 47 kDa, respectively - D1 and D2 polypeptides PS II reaction centre polypeptides encoded by the psbA and psbD genes, respectively - HPLC high performance liquid chromatography - PS II Photosystem two - SDS-PAGE sodium dodecyl sulphate-polyacrylamide gel electrophoresis - P680 primary electron donor of PS II - Pheo phenophytin a - SPC single photon counting - PBQ phenyl-p-benzoquinone - DPC 1,5-diphenylcarbazide AFRC Photosynthesis Research Group, Department of Biochemistry     

Optical absorption and fluorescence spectroscopy studies of ground state melanin-cationic porphyrins complexes.

Optical absorption and fluorescence spectroscopies were employed in the study of the interaction between synthetic L-dopa (dihydroxyphenylalanine) melanin and the cationic porphyrins tetrakis(4-N-methylpyridyl) porphyrin (TMPyP), tetrakis(4-N-benzylpyridyl)porphyrin (TBzPyP), zinc tetrakis(4-N-methylpyridyl)porphyrin (ZnTMPyP) and zinc tetrakis (4-N-benzylpyridyl)porphyrin (ZnTBzPyP). Optical absorption and fluorescence properties of the porphyrins were dependent on the symmetry of the central ring. No evidence was found for dimerization of the porphyrins in phosphate buffer, pH 7, in the concentration range between 4 x 10(-8) to 5 x 10(-5) M. Addition of L-dopa melanin red shifted the optical absorption spectra of porphyrins, concomitant to broadening and reduction in intensity of the bands. L-Dopa melanin also strongly quenched the fluorescence of the porphyrins. Time resolution of the fluorescence decay of porphyrins showed at least two lifetimes that were only slightly modified in the presence of melanin. The interaction between melanin and porphyrin resulted in the formation of non-fluorescent ground state complexes. It was found that there are two different classes of binding sites in melanin for complexation with cationic porphyrins and the values of dissociation constants are of the order of 10(-8) M. These values and the number of binding sites are dependent on the nature of the porphyrins. It was shown that the binding has electrostatic origin, but it is also affected by metal coordination and hydrophobic interaction.     

Confirmation that multiexponential fluorescence decay behavior of holoazurin originates from conformational heterogeneity

Homologous azurins from Pseudomonas fluorescens (ATCC 13525) and Pseudomonas aeruginosa (ATCC 10145) were examined by a number of electrophoretic techniques, and their copper to protein stoichiometry was determined by atomic absorption and amino acid analysis. Provided that the spectral ratio (A620/A280 or A625/A280) was 0.53 and there was no evidence of a Soret band in the absorption spectrum, then these criteria can be used to judge the homogeneity of the azurin sample. If the spectral ratio was less than 0.50, evidence suggested a nonreconstitutable, non-trypsin-digestible apoazurin was present. The fluorescence decay of these homogeneous holoazurins included three components, not two as previously reported [Szabo, A. G., et al. (1983) Biophys. J. 41, 233-244]. Whereas the decay times were nearly the same for the azurins from the different sources, the fractional fluorescence of each component varied with the azurin measured. The fluorescence of the corresponding apoazurins, prepared by a refined procedure, obeyed monoexponential decay kinetics. The temperature and pH effects on the fluorescence behavior of these homologous azurins are presented with the pH study suggesting an influence by a group which titrates between pH 5 and pH 7. When taken together these results confirm that the multiexponential decay behavior originates from conformational heterogeneity and not from contamination by an apo form.     

Tryptophan side chain conformers monitored by NMR and time-resolved fluorescence spectroscopies

We have inserted a tryptophan (F77W) in the core of the regulatory domain of cardiac troponin C (cNTnC), and previously determined the structure of this mutant with and without the cosolvent trifluoroethanol (TFE). Interestingly, the orientations of the indole side chain of the Trp are in opposite directions in the two structures (Julien et al., Protein Sci 2009; 18:1165-1174). Fluorescence decay experiments for single Trp-containing proteins often show several lifetimes, which have been interpreted as reflecting conformational heterogeneity of the Trp side chain resulting from different rotamers. To test this interpretation, we monitored the effect of TFE on wild type, F77W and F77W-V82A calcium-saturated cNTnC using 2D (13)C-HSQC NMR and time-correlated single photon counting fluorescence spectroscopies. The time dependence of the Trp fluorescence decay was fit with three lifetimes. Addition of TFE caused a gradual, but limited decrease of the lifetimes due to dynamic quenching. For F77W cNTnC, the amplitude fractions of the lifetimes also changed upon addition of TFE-the long lifetime increased from 13 to 29%, while the middle lifetime decreased from 63 to 50% and the short lifetime remained relatively unchanged. For F77W-V82A cNTnC, comparable NMR changes are observed, confirming the switch in rotamer conformation, but only much smaller changes in fluorescence decay parameters were detected. These data indicate that the balance between the rotamer states can be changed without changing the lifetime amplitude fractions appreciably, and suggest that the environment(s) of the indole ring, responsible for the different lifetimes, can result from factors other than the intrinsic rotamer state of the tryptophan.     

Chlorophyll b to chlorophyll a energy transfer kinetics in the CP29 antenna complex: a comparative femtosecond absorption study between native and reconstituted proteins

The energy transfer processes between Chls b and Chls a have been studied in the minor antenna complex CP29 by femtosecond transient absorption spectroscopy. Two samples were analyzed: the native CP29, purified from higher plants, and the recombinant one, reconstituted in vitro with the full pigment complement. The measurements indicate that the transfer kinetics in the two samples are virtually identical, confirming that the reconstituted CP29 has the same spectroscopic properties as the native one. In particular, three lifetimes (150 fs, 1.2 ps, and 5-6 ps) were identified for Chl b-652 nm to Chl a energy transfer and at least one for Chl b-640 nm (600-800 fs). Considering that the complexes bind two Chls b per polypeptide, the observation of more than two lifetimes for the Chl b to Chl a energy transfer, in both samples, clearly indicates the presence of the so-called mixed Chl binding sites--sites which are not selective for Chl a or Chl b, but can accommodate either species. The kinetic components and spectra are assigned to specific Chl binding sites in the complex, which provides further information on the structural organization.     

Conformational dynamics of bovine Cu, Zn superoxide dismutase revealed by time-resolved fluorescence spectroscopy of the single tyrosine residue.

The structural dynamics of bovine erythrocyte Cu, Zn superoxide dismutase (BSOD) was studied by time-resolved fluorescence spectroscopy. BSOD is a homodimer containing a single tyrosine residue (and no tryptophan) per subunit. Frequency-domain fluorometry revealed a heterogeneous fluorescence decay that could be described with a Lorentzian distribution of lifetimes. The lifetime distribution parameters (center and width) were markedly dependent on temperature. The distribution center (average lifetime) displayed Arrhenius behavior with an Ea of 4.2 kcal/mol, in contrast with an Ea of 7.4 kcal/mol for the single-exponential decay of L-tyrosine. This indicated that thermal quenching of tyrosine emission was not solely responsible for the effect of temperature on the lifetimes of BSOD. The distribution width was broad (1 ns at 8 degrees C) and decreased significantly at higher temperatures. Furthermore, the width of the lifetime distribution increased in parallel to increasing viscosity of the medium. The combined effects of temperature and viscosity on the fluorescence decay suggest the existence of multiple conformational substrates in BSOD that interconvert during the excited-state lifetime. Denaturation of BSOD by guanidine hydrochloride produced an increase in the lifetime distribution width, indicating a larger number of conformations probed by the tyrosine residue in the denatured state. The rotational mobility of the tyrosine in BSOD was also investigated. Analysis of fluorescence anisotropy decay data enabled resolution of two rotational correlation times. One correlation time corresponded to a fast (picosecond) rotation that contributed 62% of the anisotropy decay and likely reported local mobility of the tyrosine ring. The longer correlation time was 50% of the expected value for rotation of the whole (dimeric) BSOD molecule and appeared to reflect segmental motions in the protein in addition to overall tumbling. Comparison between rotational correlation times and fluorescence lifetimes of BSOD indicates that the heterogeneity in lifetimes does not arise from mobility of the tyrosine per se, but rather from dynamics of the protein matrix surrounding this residue which affect its fluorescence decay.     

Time-resolved extrinsic fluorescence of aromatic-L-amino-acid decarboxylase

The coenzyme-linked fluorescence of aromatic-L-amino-acid decarboxylase decays non-exponentially. The decay of both native and NaBH4 reduced samples can only be fitted by two exponentials each roughly accounting for about half of the total fluorescence. Denaturation of the reduced protein with 8 M urea makes the fluorescence decay mono-exponential, like that observed for the reference compound pyridoxamine-5-phosphate. An extra pyridoxyl moiety can be bound to the enzyme after incubation with excess pyridoxal phosphate and reduction with NaBH4. This sample is almost twice as fluorescent and shows also two lifetimes. After denaturation only one fluorescence lifetime is observed. The presence of two non-equivalent pyridoxal sites in the native enzyme can be postulated. The heterogeneous decay behaviour of the pyridoxyl moiety in the enzyme together with the variability of lifetime shown, makes this fluorophore an even more interesting fluorescent probe for proteins.     

Fluorescence lifetime spectroscopy in multiply scattering media with dyes exhibiting multiexponential decay kinetics

To investigate fluorescence lifetime spectroscopy in tissue-like scattering, measurements of phase modulation as a function of modulation frequency were made using two fluorescent dyes exhibiting single exponential decay kinetics in a 2% intralipid solution. To experimentally simulate fluorescence multiexponential decay kinetics, we varied the concentration ratios of the two dyes, 3,3-diethylthiatricarbocyanine iodide and indocynanine green (ICG), which exhibit distinctly different lifetimes of 1.33 and 0.57 ns, respectively. The experimental results were then compared with values predicted using the optical diffusion equation incorporating 1) biexponential decay, 2) average of the biexponential decay, as well as 3) stretched exponential decay kinetic models to describe kinetics owing to independent and quenched relaxation of the two dyes. Our results show that while all kinetic models could describe phase-modulation data in nonscattering solution, when incorporated into the diffusion equation, the kinetic parameters failed to likewise predict phase-modulation data in scattering solutions. We attribute the results to the insensitivity of phase-modulation measurements in nonscattering solutions and the inaccuracy of the derived kinetic parameters. Our results suggest the high sensitivity of phase-modulation measurements in scattering solutions may provide greater opportunities for fluorescence lifetime spectroscopy.     

Temperature dependence of tryptophan fluorescence lifetime in aqueous glycerol and trehalose solutions

The temperature dependences of tryptophan fluorescence decay kinetics in aqueous glycerol and 1 M trehalose solutions were examined. The fluorescence decay kinetics were recorded in the spectral region of 292.5–417.5 nm with nanosecond time resolution. The kinetics curves were approximated by the sum of three exponential terms, and the spectral distribution (DAS) of these components was determined. An antisymbatic course of fluorescence decay times of two (fast and medium) components in the temperature range from –60 to +10°C was observed. The third (slow) component showed only slight temperature dependence. The antisymbatic behavior of fluorescence lifetimes of the fast and medium components was explained on the assumption that some of the excited tryptophan molecules are transferred from a short-wave-length B-form with short fluorescence lifetime to a long-wavelength R-form with an intermediate fluorescence lifetime. This transfer occurred in the indicated temperature range.