Decay kinetics and quantum yields of fluorescence in photosystem I from Synechococcus elongatus with P700 in the reduced and oxidized state: are the kinetics of excited state decay trap-limited or transfer-limited?

Transfer and trapping of excitation energy in photosystem I (PS I) trimers isolated from Synechococcus elongatus have been studied by an approach combining fluorescence induction experiments with picosecond time-resolved fluorescence measurements, both at room temperature (RT) and at low temperature (5 K). Special attention was paid to the influence of the oxidation state of the primary electron donor P700. A fluorescence induction effect has been observed, showing a approximately 12% increase in fluorescence quantum yield upon P700 oxidation at RT, whereas at temperatures below 160 K oxidation of P700 leads to a decrease in fluorescence quantum yield ( approximately 50% at 5 K). The fluorescence quantum yield for open PS I (with P700 reduced) at 5 K is increased by approximately 20-fold and that for closed PS I (with P700 oxidized) is increased by approximately 10-fold, as compared to RT. Picosecond fluorescence decay kinetics at RT reveal a difference in lifetime of the main decay component: 34 +/- 1 ps for open PS I and 37 +/- 1 ps for closed PS I. At 5 K the fluorescence yield is mainly associated with long-lived components (lifetimes of 401 ps and 1.5 ns in closed PS I and of 377 ps, 1.3 ns, and 4.1 ns in samples containing approximately 50% open and 50% closed PS I). The spectra associated with energy transfer and the steady-state emission spectra suggest that the excitation energy is not completely thermally equilibrated over the core-antenna-RC complex before being trapped. Structure-based modeling indicates that the so-called red antenna pigments (A708 and A720, i.e., those with absorption maxima at 708 nm and 720 nm, respectively) play a decisive role in the observed fluorescence kinetics. The A720 are preferentially located at the periphery of the PS I core-antenna-RC complex; the A708 must essentially connect the A720 to the reaction center. The excited-state decay kinetics turn out to be neither purely trap limited nor purely transfer (to the trap) limited, but seem to be rather balanced.     

Determination of the excited-state lifetimes of the tryptophan residues in barnase, via multifrequency phase fluorometry of tryptophan mutants.

A multifrequency phase fluorometric study is described for wild-type barnase and engineered mutant proteins in which tryptophan residues have been replaced by less fluorescent residues which do not interfere with the determination of the tryptophan emission spectra and lifetimes. The lifetimes of the three tryptophans in the wild-type protein have been resolved. Trp-35 has a single fluorescence lifetime, which varies in the different proteins between 4.3 and 4.8 ns and is pH-independent between pH 5.8 and 8.9. Trp-71 and Trp-94 behave as an energy-transfer couple with both forward and reverse energy transfer. The couple shows two fluorescence lifetimes: 2.42 (+/-0.2) and 0.74 (+/-0.1) ns at pH 8.9, and 0.89 (+/-0.05) and 0.65 (+/-0.05) ns at pH 5.8. In the mutant Trp-94----Phe the lifetime of Trp-71 is 4.73 (+/-0.008) ns at high pH and 4.70 (+/-0.004) ns at low pH. In the mutant Trp-71----Tyr, the lifetime of Trp-94 is 1.57 (+/-0.01) ns at high pH and 0.82 (+/-0.025) ns at low pH. From these lifetimes, one-way energy-transfer efficiencies can be calculated according to Porter [Porter, G.B. (1972) Theor. Chim. Acta 24, 265-270]. At pH 8.9, a 71% efficiency was found for forward transfer (from Trp-71 to Trp-94) and 36% for reverse transfer. At pH 5.8 the transfer efficiency was 86% for forward and 4% for reverse transfer (all +/-2%). These transfer efficiencies correspond fairly well with the ones calculated according to the theory of F?rster [F?rster, T. (1948) Ann. Phys. (Leipzig) 2, 55-75].(ABSTRACT TRUNCATED AT 250 WORDS)     

Nanosecond fluorescence studies of noncovalent interaction of monomeric and dimeric intercalators with DNA

The noncovalent interaction of 2-aminodipyrido[1,2-a:3',2'-d]imidazole (Glu-P-2) and its derivatives, which are potent mutagens isolated from L-glutamic acid pyrolysate, with calf thymus DNA was studied by steady-state and nanosecond fluorescence spectroscopies. The fluorescence of these compounds exhibits static quenching by noncovalent interaction with DNA. Fluorescence lifetimes of the free and intercalated states of these compounds were determined to be 9-10 and 0.5-1 ns, respectively. The bisintercalative effect of the dimeric analogue of Glu-P-2, bis(Glu-P-2)spermine (2GP-SP), to DNA was also investigated. This 2GP-SP, which has two Glu-P-2 moieties at each end of spermine, indicates a strong intramolecular interaction exhibiting remarkable quenching of fluorescence spectrum and lifetime (tau = 3.5 ns) in the absence of DNA. In the presence of DNA, however, the 3.5-ns lifetime component of fluorescence disappeared, and a two-exponential decay of fluorescence (t = approximately 10 and 1.5 ns) was observed at a DNA concentration of more than approximately 0.001 mM P, while the solution containing a very dilute DNA concentration (less than or equal to 0.001 mM P) exhibits a three-component decay of fluorescence (1.5, 3.5, and approximately 10 ns). The potent bis intercalation of two moieties in 2GP-SP with an identical DNA molecule was suggested by the DNA-concentration dependence of these fluorescence lifetimes and their intensity.     

Picosecond time-resolved study of MgCl2-induced chlorophyll fluorescence yield changes from chloroplasts

The MgCl2-induced chlorophyll fluorescence yield changes in broken chloroplasts, suspended in a cation-free medium, treated with 3,-(3',4'-dichlorophenyl)-1,1-dimethylurea and pre-illuminated, has been investigated on a pico-second time scale. Chloroplasts in the low fluorescing state showed a fluorescence decay law of the form exp --At1/2, where A was found to be 0.052 ps-1/2, and may be attributed to the rate of spillover from Photosystem II to Photosystem I. Addition of 10 mM MgCl2 produced a 50% increase in the steady-state fluorescence quantum yield and caused a marked decrease in the decay rate. The fluorescence deday law was found to be predominantly exponential with a 1/e lifetime of 1.6 ns. These results support the hypothesis that cation-induced changes in the fluorescence yield of chlorophyll are related to the variations in the rate of energy transfer from Photosystem II to Photosystem I, rather than to changes in the partitioning of absorbed quanta between the two systems.     

Fluorescence energy transfer from diphenylhexatriene to bacteriorhodopsin in lipid vesicles

Fluorescence energy transfer between the donor diphenylhexatriene (DPH) and the acceptor retinal and fluorescence depolarization of DPH are used to test current theories for fluorescence energy transfer in two-dimensional systems and to obtain information on the effect of the intrinsic membrane protein, bacteriorhodopsin, on the order and dynamics of the lipid phase. Increasing the surface concentration of acceptors by raising the protein to lipid ratio leads to a decrease in the mean fluorescence lifetime by up to a factor of four. When the acceptor concentration is reduced at a fixed protein to lipid ratio by photochemical destruction of retinal, the lifetime increases and reaches approximately the value observed in protein-free vesicles when the bleaching is complete. The shape of the decay curve and the dependency of the mean lifetime on the surface concentration of acceptors are in agreement with theoretical predictions for a two-dimensional random distribution of donors and acceptors. From this analysis a distance of closest approach between donors and acceptors of approximately 18 A is obtained, which is close to the effective radius of bacteriorhodopsin (17 A) and consistent with current ideas about the location of retinal in the interior of the protein. In the absence of energy transfer (bleached vesicles), the steady-state fluorescence anisotropy, -r, of DPH is considerably lower than in the corresponding unbleached vesicles, indicating that the effect of energy transfer must be taken into account when interpreting -r in terms of order and dynamics.     

Dimerization and inter-chromophore distance of Cph1 phytochrome from Synechocystis,as monitored by fluorescence homo and hetero energy transfer

We investigated the dimerization of phytochrome Cph1 from the cyanobacterium Synechocystis by fluorescence resonance energy transfer (FRET). As donor we used the chromophore analogue phycoerythrobilin (PEB) and as acceptor either the natural chromophore phycocyanobilin (PCB; hetero transfer) or PEB (homo transfer). Both chromophores bind in a 1:1 stoichiometry to apo-monomers expressed in Escherichia coli. Energy transfer was characterized by time-resolved fluorescence intensity and anisotropy decay after excitation of PEB by picosecond pulses from a tunable Ti-sapphire laser system. ApoCph1 was first assembled with PEB at a low stoichiometry of 0.1. The remaining sites were then sequentially titrated with PCB. In the course of this titration, the mean lifetime of PEB decreased from 3.33 to 1.25 ns in the P(r) form of Cph1, whereas the anisotropy decay was unaffected. In the P(fr)/P(r) photoequilibrium (about 65% P(fr)), the mean lifetime decreased significantly less, to 1.67 ns. These observations provide strong support for inter-chromophore hetero energy transfer in mixed PEB/PCB dimers. The reduced energy transfer in P(fr) may be due to a structural difference but is at least in part due to the difference in spectral overlap, which was 4.1 x 10(-13) and 1.6 x 10(-13) cm(3) M(-1) in P(r) and P(fr), respectively. From the changes in the mean lifetime, rates of hetero energy transfer of 0.68 and 0.37 ns(-1) were calculated for the P(r) form and the P(fr)/P(r) photoequilibrium, respectively. Sequential titration of apo Cph1 with PEB alone to full occupancy did not affect the intensity decay but led to a substantial increase in depolarization. This is the experimental signature of homo energy transfer. Values for the rate of energy transfer k(HT) (0.47 ns(-1)) and the angle 2theta between the transition dipole moment directions (2theta = 45 +/- 5 degrees) were determined from an analysis of the concentration dependence of the anisotropy at five different PEB/Cph1 stoichiometries. The independently determined rates of hetero and homo energy transfer are thus of comparable magnitude and consistent with the energy transfer interpretation. Using these results and exploiting the 2-fold symmetry of the dimer, the chromophore-chromophore distance R(DA) was calculated and found to be in the range 49 A < R(DA) < 63 A. Further evidence for energy transfer in Cph1 dimers was obtained from dilution experiments with PEB/PEB dimers: the lifetime was unchanged, but the anisotropy increased as the dimers dissociated with increasing dilution. These experiments allowed a rough estimate of 5 +/- 3 microM for the dimer dissociation constant. With the deletion mutant Cph1Delta2 that lacks the carboxy terminal histidine kinase domain less energy transfer was observed suggesting that in this mutant dimerization is much weaker. The carboxy terminal domain of Cph1 that is involved in intersubunit trans-phosphorylation and signal transduction thus plays a dominant role in the dimerization. The FRET method provides a sensitive assay to monitor the association of Cph1 monomers.     

Energy transfer and charge separation kinetics in photosystem I: Part 1: Picosecond transient absorption and fluorescence study of cyanobacterial photosystem I particles

The energy transfer and charge separation kinetics of a photosystem I (PS I) core particle of an antenna size of 100 chlorophyll/P700 has been studied by combined fluorescence and transient absorption kinetics with picosecond resolution. This is the first combined picosecond study of transient absorption and fluorescence carried out on a PS I particle and the results are consistent with each other. The data were analyzed by both global lifetime and global target analysis procedures. In fluorescence major lifetime components were found to be 12 and 36 ps. The shorter-lived one shows a negative amplitude at long wavelengths and is attributed to an energy transfer process between pigments in the main antenna Chl pool and a small long-wavelength Chl pool emitting around 720 nm whereas the longer-lived component is assigned to the overall charge separation lifetime. The lifetimes resolved in transient absorption are 7-8 ps, 33 ps, and [unk]1 ns. The shortest-lived one is assigned to energy transfer between the same pigment pools as observed also in fluorescence kinetics, the middle component of 33 ps to the overall charge separation, and the long-lived component to the lifetime of the oxidized primary donor P700⁺. The transient absorption data indicate an even faster, but kinetically unresolved energy transfer component in the main Chl pool with a lifetime <3 ps. Several kinetic models were tested on both the fluorescence and the picosecond absorption data by global target analysis procedures. A model where the long-wave pigments are spatially and kinetically connected with the reaction center P700 is favored over a model where P700 is connected more closely with the main Chl pool. Our data show that the charge separation kinetics in these PS I particles is essentially trap limited. The relevance of our data with respect to other time-resolved studies on PS I core particles is discussed, in particular with respect to the nature and function of the long-wave pigments. From the transient absorption data we do not see any evidence for the occurrence of a reduced Chl primary electron acceptor, but we also can not exclude that possibility, provided that reoxidation of that acceptor should occur within a time <40 ps.     

Frequency domain measurements of the fluorescence lifetime of ribonuclease T1.

Using multifrequency phase/modulation fluorometry, we have studied the fluorescence decay of the single tryptophan residue of ribonuclease T1 (RNase T1). At neutral pH (7.4) we find that the decay is a double exponential (tau 1 = 3.74 ns, tau 2 = 1.06 ns, f1 = 0.945), in agreement with results from pulsed fluorometry. At pH 5.5 the decay is well described by a single decay time (tau = 3.8 ns). Alternatively, we have fitted the frequency domain data by a distribution of lifetimes. Temperature dependence studies were performed. If analyzed via a double exponential model, the activation energy for the inverse of the short lifetime component (at pH 7.4) is found to be 3.6 kcal/mol, as compared with a value of 1.0 kcal/mol for the activation energy of the inverse of the long lifetime component. If analyzed via the distribution model, the width of the distribution is found to increase at higher temperature. We have also repeated, using lifetime measurements, the temperature dependence of the acrylamide quenching of the fluorescence of RNase T1 at pH 5.5. We find an activation energy of 8 kcal/mol for acrylamide quenching, in agreement with our earlier report.     

Luminescence energy transfer with lanthanide chelates: interpretation of sensitized acceptor decay amplitudes

Lanthanide chelates used as donors offer several advantages over classical fluorescence probes in resonance energy transfer distance measurements. One of these advantages is that energy transfer can be conveniently measured using sensitized acceptor decay measurements. In these measurements a long microsecond lifetime of the lanthanide donor and a short nanosecond lifetime of the acceptor allow elimination of a signal from the unquenched donor. Therefore, the decay of sensitized acceptor emission reflects decay properties of the donor engaged in energy transfer. The purpose of this work is to point out the importance of the fact that the amplitude of the sensitized acceptor signal is dependent on the resonance energy transfer rate constant. Thus, in the case where there are two or more populations of donors with different energy transfer rate constants, the relative amplitudes of corresponding decay components observed in sensitized acceptor emission do not represent the relative populations of the donors. We use simulations to show that these effects can be very significant. A minor population of donors with a high rate of energy transfer can produce sensitized acceptor decay which is dominated by a decay component corresponding to this minor donor population. Using a simple experimental system of rapid diffusion limit energy transfer between a europium chelate and Cy5 acceptor we show that the predicted dependency of sensitized acceptor decay amplitude on the energy transfer rate is indeed observed. We suggest that the relative importance of decay components observed in sensitized acceptor emission should be evaluated after an appropriate correction of their values such that they properly reflect possible different populations of donors. We describe a method to perform such correction.     

Distance between the agonist and noncompetitive inhibitor sites on the nicotinic acetylcholine receptor

The nicotinic acetylcholine receptor possesses an agonist binding site on each of the two alpha-subunits and an allosterically coupled noncompetitive inhibitor (NCI) site. The spatial relationships between these sites have been determined by fluorescence energy transfer employing lifetime and steady-state techniques with two donor-acceptor pairs. 6-(5-Dimethylaminonaphthalene-1-sulfonamido)hexanoic acid-beta-(N-trimethylammonium)ethyl ester (dansyl-C6-choline, an agonist) and bis(choline)-N-(4-nitrobenzo-2-oxa-1,3-diazol-7-yl)-iminodiprop rionate (BCNI, a competitive antagonist) were employed as energy donors bound to the agonist sites. Ethidium was employed as a specific probe of the NCI site and served as the energy acceptor for both donors. Under steady-state conditions, energy transfer was measured by monitoring BCNI fluorescence as a function of occupancy of ethidium. Changes in acceptor occupancy were achieved by titrating acetylcholine receptor-donor-acceptor complexes with phencyclidine, a nonfluorescent NCI ligand. Extrapolation of the data to 100% acceptor occupancy yielded a transfer efficiency of 38% for the BCNI-ethidium pair. In the second method, the transfer efficiency of the dansyl-C6-choline-ethidium pair was determined by analysis of the reduction of the donor-excited state fluorescence lifetime. The nanosecond decay rates for dansyl-C6-choline measured in the presence of phencyclidine are characterized by two lifetimes (tau 1 = 6.7; tau 2 = 17.1 ns) with an amplitude ratio, alpha 1/alpha 2 = 2.3. In the presence of ethidium, the two lifetimes were proportionally diminished while retaining a comparable ratio of amplitudes. Displacement of ethidium from the NCI site by phencyclidine restored the two lifetimes to their original values. These data indicate that the donors bound to the two agonist sites transferred energy with similar efficiencies to the acceptor. Thus, the lifetime data suggest that the NCI site is approximately equidistant from each of the agonist sites. The corrected efficiency of donor quenching by this method was 34%, a value in close accord with the steady-state measurements. The distance between the agonist sites and the NCI site was calculated to be between 21-35 A for the BCNI/ethidium pair and 22-40 A for the dansyl-C6-choline/ethidium pair. Consideration of these distances with respect to the molecular dimensions of the receptor and location of the agonist sites suggests a location for the NCI site near the ion channel at the extracellular surface of the membrane bilayer.     

A new fluorescence band F689 in photosystem II revealed by picosecond analysis at 4-77 K: Function of two terminal energy sinks F689 and F695 in PS II

We performed picosecond time-resolved fluorescence spectroscopy in spinach photosystem II (PS II) particles at 4, 40, and 77 K and identified a new fluorescence band, F689. F689 was identified in addition to the well-known F685 and F695 bands in both analyses of decay-associated spectra and global Gaussian deconvolution of time-resolved spectra. Its fast decay suggests the energy transfer directly from F689 to the reaction center chlorophyll P680. The contribution of F689, which increases only at low temperature, explains the unusually broad and variable bandwidth of F695 at low temperature. Global analysis revealed the three types of excitation energy transfer/dissipation processes: (1) energy transfer from the peripheral antenna to the three core antenna bands F685, F689, and F695 with time constants of 29 and 171 ps at 77 and 4 K, respectively; (2) between the three core bands (0.18 and 0.82 ns); and (3) the decays of F689 (0.69 and 3.02 ns) and F695 (2.18 and 4.37 ns). The retardations of these energy transfer rates and the slow F689 decay rate produced the strong blue shift of the PS II fluorescence upon the cooling below 77 K.     

Picosecond time-resolved fluorescence of ribonuclease T1. A pH and substrate analogue binding study.

The tryptophyl fluorescence of ribonuclease T1 decays monoexponentially at pH 5.5, tau = 4.04 ns but on increasing pH, a second short-lived component of 1.5 ns appears with a midpoint between pH 6.5 and 7.0. Both components have the same fluorescence spectrum. Acrylamide quenches both fluorescence components, and the short-lived component is quenched fivefold faster than the predominant long component. Binding of the substrate analogue 2'-guanylic acid at pH 5.5 quenches the fluorescence by 20% and introduces a second decay component, tau = 1.16 ns. Acrylamide quenches both tryptophyl decay components, with similar quenching rates. The fluorescence anisotropy decay of ribonuclease T1 was consistent with a molecule the size of ribonuclease T1 surrounded by a single layer of water at pH 7.4, even though the anisotropy decay at pH 5.5 deviated from Stokes-Einstein behavior. The fluorescence data were interpreted with a model where the tryptophyl residue exists in two conformations, remaining in a hydrophobic pocket. The acrylamide quenching is interpreted with electron transfer theory and suggests that one conformer has the nearest atom approximately 3 A from the protein surface, and the other, approximately 2 A.     

A new fluorescence band F689 in photosystem II revealed by picosecond analysis at 4-77 K: function of two terminal energy sinks F689 and F695 in PS II

We performed picosecond time-resolved fluorescence spectroscopy in spinach photosystem II (PS II) particles at 4, 40, and 77 K and identified a new fluorescence band, F689. F689 was identified in addition to the well-known F685 and F695 bands in both analyses of decay-associated spectra and global Gaussian deconvolution of time-resolved spectra. Its fast decay suggests the energy transfer directly from F689 to the reaction center chlorophyll P680. The contribution of F689, which increases only at low temperature, explains the unusually broad and variable bandwidth of F695 at low temperature. Global analysis revealed the three types of excitation energy transfer/dissipation processes: (1) energy transfer from the peripheral antenna to the three core antenna bands F685, F689, and F695 with time constants of 29 and 171 ps at 77 and 4 K, respectively; (2) between the three core bands (0.18 and 0.82 ns); and (3) the decays of F689 (0.69 and 3.02 ns) and F695 (2.18 and 4.37 ns). The retardations of these energy transfer rates and the slow F689 decay rate produced the strong blue shift of the PS II fluorescence upon the cooling below 77 K.     

The fluorescence decay kinetics of in vivo chlorophyll measured using low intensity excitation

We report fluorescence lifetimes for in vivo chlorophyll a using a time-correlated single-photon counting technique with tunable dye laser excitation. The fluorescence decay of dark-adapted chlorella is almost exponential with a lifetime of 490 ps, which is independent of excitation from 570 nm to 640 nm.Chloroplasts show a two-component decay of 410 ps and approximately 1.4 ns, the proportion of long component depending upon the fluorescence state of the chloroplasts. The fluorescence lifetime of Photosystem I was determined to be 110 ps from measurements on fragments enriched in Photosystem I prepared from chloroplasts with digitonin.     

The fluorescence properties of a DNA probe

Steady-state and dynamic fluorescence measurements have been performed on DAPI in solution and in complexes formed with a number of synthetic and natural polydeoxynucleotides. The decay of DAPI in buffer at pH 7 was decomposed using two exponentials having lifetime values of approximately 2.8 ns and 0.2 ns. The double exponential character of the decay was maintained over a large pH range from 3 to 9. At pH 1 the short component dominated, whereas at pH 12, only the long component was detectable. Two distinct spectra were associated with the two lifetime components; the short component was shifted to the red. The short lifetime component occurs in the presence of water. In water the excitation spectra depended on the emission wavelength and there was no viscosity dependence of the two forms. To explain these results we propose that there is a ground state conformer in which preferential solvation of the indole ring allows proton transfer in the excited state. DAPI complexed with polydeoxynucleotides retained most of the features of the decay of DAPI in solution. However, the complexes with fuly AT-containing polymers stabilized the longer lifetime form of DAPI because the stronger binding enhanced solvent shielding. A gradual increase of the short lifetime component, which monitors dye solvent exposure, was obtained as the AT content was decreased. For polyd(GC) the decay was similar to that of free DAPI.Abbreviations DAPI 4-6-diamidino-2-phenylindole - POPOP 1,4-bis(5-phenyl-2-oxazolyl)-benzene; 2,2-p-phenylene-bis(5-phenyloxazole) Financial support for this work was provided by a M.P.I. grant 1984, Roma, Italy for M.L.B. and NSF-PCM 84-03107 and PHS-IP41RR03155 for E.G.     

Time-resolved fluorescence of DAPI in solution and bound to polydeoxynucleotides

Fluorescence decay studies, obtained by multifrequency phase-modulation fluorometry, have been performed on DAPI in solution and complexed with natural and synthetic polydeoxynucleotides. DAPI decay at pH 7 was decomposed using two exponential components of 2.8 and 0.2 ns of lifetime values, respectively. The double exponential character of the decay was maintained over a large pH range. Phase- and modulation-resolved spectra, collected between 420 and 550 nm, have indicated at least two spectral components associated with the two lifetime values. This, plus the observation of the dependence of the emission spectrum on the excitation wavelength, suggests a lifetime heterogeneity originating from ground-state molecular conformers, partially affected by pH changes. DAPI complexed with natural polydeoxynucleotides retained most of the features of DAPI decay in solution, except for the value of the long lifetime component that was longer (approximately 4 ns) and the relative fractional fluorescence intensities of the two components that were inverted. AT polymers/DAPI complexes show single exponential decay. Solvent shielding when DAPI is bound to DNA changes the indole ring solvation and stabilizes the longer lifetime decay component. For poly(GC)/DAPI complex, the decay was similar to that of free DAPI in solution, proving the dependence on the polydeoxynucleotides sequence the different types of binding and the reliability of the fluorescence method to solve them.     

Effect of proteins on fluorophore lifetime heterogeneity in lipid bilayers.

The effect of three different membrane proteins on the fluorescence lifetime heterogeneity of 1,6-diphenyl-1,3,5-hexatriene (DPH) in phospholipid vesicle systems was investigated. For large unilamellar vesicles of dimyristoylphosphatidylcholine (DMPC) and 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) at 37 degrees C, the fluorescence decay was essentially monoexponential (8.6 and 8.2 ns, respectively) except for a minor component typical of DPH. For gramicidin D reconstituted into DMPC vesicles at a protein/lipid molar ratio of 1/7, the most appropriate analysis of the data was found to be in the form of a bimodal Lorentzian distribution. Centers of the major lifetime components were almost identical with those recovered for vesicles without proteins, while broad distributional widths of some 4.0 ns were recovered. Variation of the protein/lipid molar ratio in sonicated POPC vesicles revealed an abrupt increase in distributional width at ratios approximating 1/15-1/20, which leveled off at about 2.5 ns. For bacteriorhodopsin in DMPC vesicles and cytochrome b5 in POPC, the most appropriate analysis of the data was again found to be in the form of a bimodal Lorentzian also with broad distributional widths in the major component. Lifetime centers were decreased for these proteins due to fluorescence energy transfer to the retinal of the bacteriorhodopsin and heme of the cytochrome b5. Fluorescence energy transfer is distance dependent, and since a range of donor-acceptor distances would be expected in a membrane, lifetime distributions should therefore be recovered independently of other effects for proteins possessing acceptor chromophores.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fluorescence study of the ligand stereospecificity for binding to lumazine protein.

6,7-Dimethyllumazine derivatives, substituted at the 8-position with aldityls or monohydroxyalkyl groups, have been examined for their binding ability to lumazine apo-protein from two strains of Photobacterium phosphoreum using fluorescence dynamics techniques. On the protein the lumazine has a nearly monoexponential decay of fluorescence with lifetime 13.8 ns (20 degrees C). In free solution the lifetime is 9.6 ns. The concentration of free and bound lumazine in an equilibrium mixture can be recovered readily by analysis of the fluorescence decay. Only the aldityl derivatives D-xylityl and 3'-deoxy-D-ribityl, having stereoconfigurations at the 2' and 4' positions identical to the natural ligand, 8-(1'-D-ribityl), show comparable dissociation constants (0.3 microM, 20 degrees C, pH 7.0). D-Erythrityl and L-arabityl have dissociation constants of 1-2 microM. All other ligands show no interaction at all or have dissociation constants in the range 6-80 microM, which can still be determined semi-quantitatively using the fluorescence decay technique. In the case of these very weakly bound ligands, unambiguous detection of bound ligand can be shown by a long correlation time (23 ns, 2 degrees C) for the fluorescence anisotropy decay. Examination of the bound D-xylityl compound's fluorescence anisotropy decay at high time resolution (< 100 ps) shows rigid association, i.e. no mobility independent of the macromolecule. All bound ligands appear to be similarly positioned in the binding site. The influence of the stereoconfiguration at the 8-position found for lumazine protein parallels that previously observed for the enzyme riboflavin synthase, where the lumazines are substrates or inhibitors. This is consistent with the finding of significant sequence similarity between these proteins. The binding rigidity may have implications for the mechanism of the enzyme.     

不同pH条件下R-藻红蛋白和C-藻蓝蛋白荧光寿命的研究

采用自己研制的时间分辨毫微秒荧光谱仪对R-藻红蛋白(R-PE )和C-藻蓝蛋白(C-PC)进行了荧光寿命的测定和研究,并对能量传递过程进行了分析和讨论.测得R-PE的荧光寿命为3.1±0.1ns,C-PC的荧光寿命为1.3±0.1ns,且在pH5—pH9的范围内不变;当pH<5时,两者的荧光寿命都有变短的趋势.我们还测定了R-PE和C-PC混合溶液中R-PE的荧光寿命不变,而C-PC的荧光寿命变长,从而表明存在着R-PE向C-PC的辐射能量传递.