Interpretation of intramolecular stacking effect on the fluorescence intensity decay of 3-methylbenzimidazolyl(5′-5′)guanosine dinucleotides using a model of lifetime distribution

Time-resolved fluorescence of 3-methylbenzimidazole (m³B) was used to study stacking interaction between base moieties in di-, tri- and tetra-phosphate analogues of 3-methylbenzimidazolyl(5′-5′)guanosine (m³Bp _n G, n = 2, 3, 4), using 5′-triphosphate of 3-methylbenzimidazole riboside (m³BTP) as reference. Fluorescence intensity decays of all compounds cannot be satisfactory fitted with single-exponential function. Although an increase of a number of exponents led to better fits, interpretation of the individual exponential terms, i.e. pre-exponential amplitudes and fluorescence lifetimes, cannot be adequately characterized. We show that these fluorescence decays are best fitted by power-like function derived from physically justified distribution of the fluorescence lifetimes, and characterized by the mean value of the excited-state lifetime and relative variance of lifetime fluctuations around the mean value. The latter led to the parameter of heterogeneity and number of decay paths, which depend on the factors responsible for non-radiative decay of the excited state, including base–base stacking interaction. This was studied by means of changes of temperature and the number of phosphate groups in dinucleotides. It was shown that the strongest effect of stacking interactions, characterized by lowest values of both fluorescence mean decay time and relative variance, occurs in the case of m³Bp₃G containing the same number of phosphates as natural mRNA cap. The possible importance of these results for interpretation of the mechanism of function of the mRNA cap structure is discussed.     

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.     

Application of a reference convolution method to tryptophan fluorescence in proteins. A refined description of rotational dynamics

A reference method for the deconvolution of polarized fluorescence decay data is described. Fluorescence lifetime determinations for p-terphenyl, p-bis[2-(5-phenyloxazolyl)]benzene and N-acetyltryptophanamide (AcTrpNH2) show that with this method more reliable fits of the decays can be made than with the scatterer method, which is most frequently used. Analysis of the AcTrpNH2 decay with p-terphenyl as the reference compound yields an excellent fit with lifetimes of 2.985 ns for AcTrpNH2 and 1.099 ns for p-terphenyl (20 degrees C), whereas the AcTrpNH2 decay cannot be satisfactorily fitted when the scatterer method is used. The frequency of the detected photons is varied to determine the conditions where pulse pile-up starts to affect the measured decays. At detection frequencies of 5 kHz and 15 kHz, which corresponds to 1.7% and 5% respectively of the rate of the excitation photons no effects are found. Decays measured at 30 kHz (10%) are distorted, indicating that pile-up effects play a role at this frequency. The fluorescence and fluorescence anisotropy decays of the tryptophan residues in the proteins human serum albumin, horse liver alcohol dehydrogenase and lysozyme have been reanalysed with the reference method. The single tryptophan residue of the albumin is shown to be characterized by a triple-exponential fluorescence decay. The anisotropy decay of albumin was found to be mono-exponential with a rotational correlation time of 26 ns (20 degrees C). The alcohol dehydrogenase has two different tryptophan residues to which single lifetimes are assigned. It is found that the rotational correlation time for the dehydrogenase changes with excitation wavelength (33 ns for lambda ex = 295 nm and 36 ns for lambda ex = 300 nm at 20 degrees C), indicating a nonspherical protein molecule. Lysozyme has six tryptophan residues, which give rise to a triple-exponential fluorescence decay. A single-exponential decay with a rotational correlation time of 3.8 ns is found for the anisotropy. This correlation time is significantly shorter than that arising from the overall rotation and probably originates from intramolecular, segmental motion.     

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.     

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.     

Phenylalanine-to-tyrosine singlet energy transfer in the archaebacterial histone-like protein HTa

The Archaebacterium Thermoplasma acidophilum has a histone-like protein (HTa) abundantly associated with its deoxyribonucleic acid. Each native tetrameric complex of HTa contains 20 phenylalanine residues, 4 tyrosine residues, and no tryptophan. When the protein was excited by radiation at 252 nm, which is a wavelength absorbed predominantly by phenylalanine, the fluorescent emission was mostly from tyrosine. According to the excitation spectrum for this tyrosine fluorescence, the cause was energy transfer from phenylalanine, which occurred with about 50% efficiency. When the tyrosine residues were removed enzymatically, the excited-state lifetime of the phenylalanine residues nearly doubled. Because of energy transfer, the tyrosine emission had two apparent fluorescence decay lifetimes; one lifetime (3.9 ns) was that of tyrosine while the second (12.1 ns) corresponded to the excited state of phenylalanine.     

Multiple conformational states in myoglobin revealed by frequency domain fluorometry

The tryptophanyl fluorescence decays of two myoglobins, i.e., sperm whale and tuna myoglobin, have been examined in the frequency domain with an apparatus which utilizes the harmonic content of a mode-locked laser. Data analysis was performed in terms of continuous distribution of lifetime having a Lorentzian shape. Data relative to sperm whale myoglobin, which possesses two tryptophanyl residues, i.e., Trp-A-5 and -A-12, provided a broad lifetime distribution including decay rates from a few picoseconds to about 10 ns. By contrast, the tryptophanyl lifetime distribution of tuna myoglobin, which contains only Trp-A-12, showed two well-separated and narrow Lorentzian components having centers at about 50 ps and 3.37 ns, respectively. In both cases, the chi 2 obtained from distribution analysis was lower than that provided by a fit using the sum of exponential components. The long-lived components present in the fluorescence decay of the two myoglobins do not correspond to any of those observed for the apoproteins at neutral pH. The tryptophanyl lifetime distribution of sperm whale apomyoglobin consists of two separated Lorentzian components centered at 2.25 and 5.4 ns, whereas that of tuna apomyoglobin consists of a single Lorentzian component, whose center is at 2.19 ns. Acidification of apomyoglobin to pH 3.5 produced a shift of the distribution centers toward longer lifetimes.(ABSTRACT TRUNCATED AT 250 WORDS)     

Measurements of fluorescence lifetimes by use of a hybrid time-correlated and multifrequency phase fluorometer

Measurements of homogeneous and heterogeneous fluorescence intensity decays using a hybrid time-correlated single photon counting/multifrequency phase fluorometer are reported. A trio of fluorophores exhibiting a range of decay profiles was selected. p-Terphenyl, 1,4-bis[2-(4-methyl-5-phenyloxazolyl)]benzene [(Me)2POPOP], and p-bis[2-(5-phenyloxazolyl)]benzene (POPOP), commonly used reference fluorophores, were analyzed initially; their emissions were characterized by monoexponential decay functions. Additionally, emissions from two single tryptophan proteins with different decay profiles were measured. Scorpion neurotoxin variant 3 required three exponentials to fit the emission decay properly (average lifetime approximately 500 ps). At pH 5.5, the fluorescence emission of ribonuclease T1 showed a monoexponential decay with a measured lifetime of approximately 4.0 ns. Thus, in each case, the results from both measurements were consistent between the two detection systems, confirming the view that the two approaches for measuring fluorescence lifetimes are equivalent.     

Pulsefluorimetry of tyrosyl peptides

The fluorescence quantum yield and the fluorescence decay of aqueous solutions of derivatives containina a single tyrosine residue have been measured at different pH. In these derivatives tyrosine was substituted on its amino end (series I) or/and, on its carboxyl end (series II), by acyl, amino or amino acyl groups. The fluorescence decays of series I derivatives are monoexponential regardless to the ionization state of their amino group. Upon deprotonation of the α-amino group, the quantum yields and the lifetimes increase in the case of dipeptides, and slightly decrease, for the tripeptides. The quantum yield and the lifetime increase with the side chain length of the aliphatic residue adjacent to the tyrosine residue, (the fluorescence of Val Tyr anion being identical to that of free Tyrosine). Quite different is the behavior of series II derivatives: their decays at pH 5.5 must be described by two exponential terms, one of them decaying with a short time constant (about 0.5 ns) and little side chain effect is observed. The fluorescence intensity increases upon deprolonalion of the α-amino proup (though to a lesser extent than for series I derivatives); a nearly monoexponential decay is observed at basic pH for dipeptides. but not for tyrosine amide, amide or dipeptides, or tripeptides. The following interpretation of our results is proposed: fluorescence quenching occurs in molecular conformations in which a peptide carbonyl can come in contact with the phenolic chromophore. This condition depends mainly on the value of the angle x₁ which determines the conformation of the tyrosyl residue around its C_α-C_β bond. It appears that the rotamer in which quenching occurs are not the same for series I and series II derivatives, which can explain the different behavior of these two kinds of compounds. The interpretation of the fluorescence properties is developed taking into account on one side the relative population of the rotamers in the ground state, which is given by studies of crystals and of solutions, and on the other side the possibility of an exchange between these rotamers during the excited state time. In this scheme the protonated α-amino groups would act to reinforce the quenching efficiency of the carbonyl. At last it is found that the radiative lifetime of the phenolic chromophore is the same for all the compounds studies.     

The fluorescence decay of tryptophan residues in native and denatured proteins.

The fluorescence decay kinetics at different ranges of the emission spectrum is reported for 17 proteins. Out of eight proteins containing a single tryptophan residue per molecule, seven proteins display multiexponential decay kinetics, suggesting that variability in protein structure may exist for most proteins. Tryptophan residues whose fluorescence spectrum is red shifted may have lifetimes longer than 7 ns. Such long lifetimes have not been detected in any of the denatured proteins studied, indicating that in native proteins the tryptophans having a red-shifted spectrum are affected by the tertiary structure of the protein. The fluorescence decay kinetics of ten denatured proteins studied obey multiexponential decay functions. It is therefore concluded that the tryptophan residues in denatured proteins can be grouped in two classes. The first characterized by a relatively long lifetime of about 4 ns and the second has a short lifetime of about 1.5 ns. The emission spectrum of the group which is characterized by the longer lifetime is red shifted relative to the emission spectrum of the group characterized by the shorter lifetime. A comparison of the decay data with the quantum yield of the proteins raises the possibility that a subgroup of the tryptophan residues is fully quenched. It is noteworthy that despite this heterogeneity in the environment of tryptophan residues in each denatured protein, almost the same decay kinetics has been obtained for all the denatured proteins studied in spite of the vastly different primary structures. It is therefore concluded that each tryptophan residue interacts in a more-or-less random manner with other groups on the polypeptide chain, and that on the average the different tryptophan residues in denatured proteins have a similar type of environment.     

Complex fluorescence of the cyan fluorescent protein: comparisons with the H148D variant and consequences for quantitative cell imaging

We have studied the fluorescence decays of the purified enhanced cyan fluorescent protein (ECFP, with chromophore sequence Thr-Trp-Gly) and of its variant carrying the single H148D mutation characteristic of the brighter form Cerulean. Both proteins exhibit highly complex fluorescence decays showing strong temperature and pH dependences. At neutral pH, the H148D mutation leads (i) to a general increase in all fluorescence lifetimes and (ii) to the disappearance of a subpopulation, estimated to be more than 25% of the total ECFP molecules, characterized by a quenched and red-shifted fluorescence. The fluorescence lifetime distributions of ECFP and its H148D mutant remain otherwise very similar, indicating a high degree of structural and dynamic similarity of the two proteins in their major form. From thermodynamic analysis, we conclude that the multiexponential decay of ECFP cannot be simply ascribed, as is generally admitted, to the slow conformational exchange characterized by NMR and X-ray crystallographic studies [Seifert, M. H., et al. (2002) J. Am. Chem. Soc. 124, 7932-7942; Bae, J. H., et al. (2003) J. Mol. Biol. 328, 1071-1081]. Parallel measurements in living cells show that these fluorescence properties in neutral solution are very similar to those of cytosolic ECFP.     

Distributions of fluorescence decay times for parinaric acids in phospholipid membranes

Analysis of fluorescence decay data for probes incorporated into model or biological membranes invariably requires fitting to more than one decay time even though the same probe exhibits nearly single-exponential decay in solution. The parinaric acids (cis and trans) are examples of this. Data are presented for both parinaric acid isomers in dimyristoylphosphatidylcholine membranes collected to higher precision than normally encountered, and the fluorescence decays are shown to be best described by a smooth distribution of decay times rather than by a few discrete lifetimes. The temperature dependence of the fluorescence decay reveals a clear shift in the distribution to longer lifetimes associated with the membrane phase transition at 23.5 degrees C. The physical significance is that fluorescence lifetime measurements appear to reflect a physical process with a distribution of lifetimes rather than several distinct physical processes.     

Dynamic fluorescence in copper proteins Selected examples

Summary The fluorescence properties of three copper proteins, namely human superoxide dismutase,Pseudomonas aeruginosa azurin andThiobacillus versutus amicyanin have been studied. All these proteins show a non-exponential decay of fluorescence, though the tryptophanyl residues responsible for the emission are very differently located in the three proteins. All the three decays can be fitted by at least two lifetimes or better with one or two lorentzian-shaped, continuous distributions of lifetime. In each case the removal of copper affects the quantum yield of fluorescence without affecting the shape of the emission.     

Characterization of the tryptophan environments of interleukins 1 alpha and 1 beta by fluorescence quenching and lifetime measurements

The tryptophan environments of interleukins 1 alpha and 1 beta, immunomodulatory proteins with similar biological activities but only 25% sequence homology, were characterized by steady-state and dynamic fluorescence measurements. Both proteins exhibited similar emission maxima, but the emission intensity of IL-1 beta was greatly enhanced by increasing the ionic strength of the medium, whereas that of IL-1 alpha was unaffected. The two cytokines were also similarly quenched by the polar quencher acrylamide, but differences were observed for the ionic quenchers iodide and cesium. The fluorescence intensity decays of both cytokines were characterized by two (long and short) component lifetimes. However, the average lifetime of IL-1 beta (4.4 ns) was much longer than that of IL-1 alpha (1.93 ns). Taken together with the results of steady-state measurements, we suggest that the single tryptophan of IL-1 beta is statically quenched by neighboring charged residues, whereas the tryptophan fluorescence of IL-1 alpha is unaffected by ionic strength, and that the tryptophans of the two proteins have different accessibilities to ionic quenchers. The results are discussed in terms of similarities and differences in the tryptophan environments of the two proteins.     

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.     

Conformational dynamics of unfolded peptides as a function of chain length: a frequency domain fluorescence approach

The fluorescence emission decays of single-tryptophan-containing peptides of different chain lengths in their unfolded state were investigated in the frequency domain. The data were analyzed using different functions, i.e., exponential fit and probability-density functions of different shape. We found that unimodal Lorentzian distributions best describe the fluorescence decays. This finding agrees with the point of view, now broadly accepted, that rapid motions exist in polypeptides. As a consequence of this flexibility, a large variety of conformations, with an unequal perturbation of tryptophan in its excited state, is generated. The lifetime distribution center was independent of the length of the polypeptide chain but strongly related to the nature of the amino acid residues located in the proximity of the tryptophan in the primary structure. The full width at half maximum, W, of the lifetime distribution was found to be related to the length of unfolded polypeptide by the empirical logarithmic relationship W = 0.83 log n, where n indicates the number of residues. For short peptides, a single lifetime or a narrow range of lifetimes is observed because of the fast relaxation of the tryptophanyl environment. On peptide lengthening, the spectrum of conformations, which the peptide can assume, increases; this causes a complex fluorescence decay represented by a lifetime distribution. For long polypeptide chains, the motions of the regions far from tryptophan do not significantly perturb the chromophore environment.     

A model for multiexponential tryptophan fluorescence intensity decay in proteins.

Tryptophan fluorescence intensity decay in proteins is modeled by multiexponential functions characterized by lifetimes and preexponential factors. Commonly, multiple conformations of the protein are invoked to explain the recovery of two or more lifetimes from the experimental data. However, in many proteins the structure seems to preclude the possibility of multiple conformers sufficiently different from one another to justify such an inference. We present here another plausible multiexponential model based on the assumption that an energetically excited donor surrounded by N acceptor molecules decays by specific radiative and radiationless relaxation processes, and by transferring its energy to acceptors present in or close to the protein matrix. If interactions between the acceptors themselves and back energy transfer are neglected, we show that the intensity decay function contain 2N exponential components characterized by the unperturbed donor lifetime, by energy transfer rates and a probability of occurrence for the corresponding process. We applied this model to the fluorescence decay of holo- and apoazurin, ribonuclease T1, and the reduced single tryptophan mutant (W28F) of thioredoxin. Use of a multiexponential model for the analysis of the fluorescence intensity decay can therefore be justified, without invoking multiple protein conformations.     

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.     

Physical properties of the fluorescent sterol probe dehydroergosterol

Spectroscopic studies were performed on the fluorescent sterol probes ergosta-5,7,9(11),22-tetraen-3 beta-ol (dehydroergosterol) and cholesta-5,7,9(11)-trien-3 beta-ol (cholestatrienol). In most isotropic solvents, these molecules exhibited a single lifetime near 300 ps. Fluorescence lifetimes in 2-propanol were independent of emission wavelength and independent of excitation wavelength. Excited state behavior of these probes appears relatively simple. In isotropic solvents, dehydroergosterol fluorescence emission underwent at most a small Stokes shift as solvent polarity was modified. Time-resolved anisotropy decays indicated that dehydroergosterol decay was monoexponential, with rotational correlation times dependent on solvent viscosity. When incorporated into L-alpha-dimyristoylphosphatidylcholine liposomes at a concentration of 0.9 mol%, dehydroergosterol fluorescence lifetime decreased at the phase transition of this phospholipid indicating that the sterol probe was detecting physical changes of the bulk phospholipids. Furthermore, total fluorescence decays and anisotropy decays were sensitive to the environment of the sterol. Dehydroergosterol and cholestatrienol are thus useful probes for monitoring sterol behavior in biological systems.