Attempts to observe through-chain energy transfer and electron transfer on α-helical polypeptide chain

Singlet singlet energy transfer between the two terminal chromophores attached to an α-helical polypeptide chain has been studied. The transfer efficiency was satisfactorily explained by Förster's theory when the interchromophore distance was calculated from the α-helical structure. Therefore, it was concluded that no particular effect from the possible energy band structure of the α-helical conformation was detected in the end-to-end energy transfer. Similarly, end-to-end electron transfer was attempted between the electron donor acceptor pair attached to the ends of α-helcial polypeptide chain. However, no intramolecular interaction was found between the donor acceptor pair, indicating that the exciton structure of the α-helical polypeptides is not effective enough to realize through-chain electron transfer.     

Energy transfer distance measurements in immunoglobulins. III. Location of the light-heavy interchain disulfide bond in rabbit immunoglobulin G antibody

The distance between the hapten combining site and the light-heavy interchain disulfide bond in the Fab fragment of rabbit immunoglobulin G has been determined by measuring the efficiency of energy transfer between chromophores specifically attached at these sites on the molecule. The donor chromophore, Dns-Lys⁴, was non-covalently bound in the combining site of the Fab fragment of high-affinity anti-Dns antibody. The acceptor chromophore, fluorescein, was covalently attached by disulfide interchange of racemic DiFlCys with specific sulfhydryls generated by reduction. The presence of acceptor decreased the donor fluorescence lifetime from 23.6 nanoseconds to 21.6 nanoseconds. From the transfer efficiency of 8.4%, an average separation distance of 76 ± 10 Å was calculated. However, a statistical analysis of the molar concentrations of donor and acceptor on Fab fragments showed that approximately equal numbers of Fab probably contained donor but no acceptor on the one hand, and both donor and acceptor on the other hand. The presence of the former subpopulation would result in an average measured efficiency of energy transfer that would be too low. Treatment of the decay data by a double-exponential analysis which took account of these two populations of Fab fragments, led to a transfer efficiency of 20% and a correspondingly shorter separation distance of 64 ± 10 Å. The latter value is to be preferred. From the results presented here, and those reported previously on the location of the combining site at the tip of the Fab fragment and of the interheavy chain disulfide bond (Bunting &; Cathou, 1973), a general summary of the dimensions of rabbit immunoglobulin G Fab is given.     

The distances separating Tyr-69 from the high-affinity nucleotide and metal binding sites in actin

The nucleotide binding site in actin was occupied with the fluorescent analogue formycin A 5' triphosphate which acted as a fluorescent donor for the acceptor chromophore dansyl chloride attached to Tyr-69. The distance separating the two chromophores was calculated to be 2.1 nm from the fluorescence energy transfer measurements. Similar measurements were made of the distances separating dansyl chloride, acting as donor, on Tyr-69 from Co2+ occupying the metal binding site. A distance of 2.1 nm was similarly obtained.     

Fluorescence energy transfer between active sites in aspartate transaminase.

The method of fluorescence energy transfer has been used to measure the distance between the active sites in a dimeric enzyme, aspartate aminotransferase. The procedure involves the prior preparation of a hybrid enzyme with the natural chromophore, pyridoxal phosphate, in one subunit as the aldimine and of the reduced aldimine in the other subunit. The two active site chromophores are used as donor and acceptor of the energy transfer and a distance of 21 Å is obtained for the separation of the active sites.     

Energy transfer distance measurements in immunoglobulins. II. Localization of the hapten binding sites and the interheavy chain disulfide bond in rabbit antibody

The distance between the hapten combining site and the single interheavy chain disulfide bond in rabbit immunoglobulin G has been determined by measuring the efficiency of energy transfer between chromophores specifically attached at these sites on the molecule. The donor chromophore, DnsLys³, was non-covalently bound in the combining sites of high-affinity antiDns antibody molecules, in one case, and in the combining site of the pepsin Fab′ fragment of antiDns in another. The acceptor chromophore, fluorescein, was covalently attached by disulfide interchange of di-FlCys with sulfhydryls generated by selective reduction of the interheavy chain disulfide bond of whole antiDns antibody and of the (Fab′)₂ pepsin fragment. The presence of acceptor decreased the donor fluorescence lifetime by about 1.0 nanosecond in both cases, i.e. for the whole antibody, from 23.6 to 22.7 nanoseconds, and for the Fab′ fragment from 23.6 to 22.5 nanoseconds. An average separation distance of 81 Å was calculated from an average observed transfer efficiency of 3.7%. This value agrees closely with the over-all length of a Fab′ fragment of a human IgG myeloma protein (Poljak et al., 1972). These results strongly suggest that the antibody combining site is at, or very close to, the tip of the Fab fragment and that the inter-heavy chain disulfide bond is at or near the edge of the C_L?C_H1 domain.     

Consideration of dipole orientation angles yields accurate rate equations for energy transfer in the rapid diffusion limit.

Dipole-dipole energy transfer between suitable donor and acceptor chromophores is an important luminescence quenching mechanism and has been shown to be useful for distance determination at the molecular level. In the rapid diffusion limit, where the excited-state lifetime of the donor is long enough to allow the donor and acceptor to diffuse many times their average separation before deexcitation, it is usually assumed that the relative dipolar orientation is completely averaged due to rotational Brownian motion. Under this simplifying assumption, analytical expressions have been derived earlier for the energy transfer rate between donor and acceptor characterized by different geometries. Most such expressions, however, are only approximate because complete angular averaging is permitted only in a geometry that possesses spherical symmetry surrounding each chromophore. In this paper analytical expressions that correctly account for incomplete angle averaging due to steric hindrance are presented for several geometries. Each of the equations reveals a dependence of the energy transfer rate on chromophore orientation. It is shown that correctly accounting for this effect can lead to improvements in estimates of the distance of closest approach from measured quenching rates based on energy transfer experiments.     

Location and orientation of the chromophore in bacteriorhodopsin: Analysis by fluorescence energy transfer

The spatial location and orientation of the retinal chromophore in bacteriorhodopsin were estimated from a fluorescence energy transfer study. The energy donor used in this study was a fluorescent retinal derivative, which was obtained by partial reduction of the purple membrane with sodium borohydride, and the energy acceptor was the native chromophore remaining in the same membrane. Since bacteriorhodopsin forms a two-dimensional crystal with P₃ symmetry in the purple membrane, and the membrane structure is maintained after the reduction, the rate of energy transfer from a donor to any acceptor existing in the same membrane can be calculated as a function of the location and orientation of the chromophores in the unit cell. Quantitative analyses of the fluorescence decay curve and the quantum yield, with various extents of reduction, enabled us to determine the most probable location and orientation. The result suggested that the chromophore was situated near the centre of the protein in such an orientation that the dipole-dipole interaction with neighbouring chromophores was close to minimum.     

Single-molecule spectroscopy selectively probes donor and acceptor chromophores in the phycobiliprotein allophycocyanin

We report on single-molecule fluorescence measurements performed on the phycobiliprotein allophycocyanin (APC). Our data support the presence of a unidirectional F?rster-type energy transfer process involving spectrally different chromophores, alpha84 (donor) and beta84 (acceptor), as well as of energy hopping amongst beta84 chromophores. Single-molecule fluorescence spectra recorded from individual immobilized APC proteins indicate the presence of a red-emitting chromophore with emission peaking at 660 nm, which we connect with beta84, and a species with the emission peak blue shifted at 630 nm, which we attribute to alpha84. Polarization data from single APC trimers point to the presence of three consecutive red emitters, suggesting energy hopping amongst beta84 chromophores. Based on the single-molecule fluorescence spectra and assuming that emission at the ensemble level in solution comes mainly from the acceptor chromophore, we were able to resolve the individual absorption and emission spectra of the alpha84 and beta84 chromophores in APC.     

Fluorescence energy transfer studies of transmembrane location of retinal in purple membrane

A diffusion-enhanced energy transfer technique was employed for the determination of transmembrane location of the retinal chromophore in the purple membrane. Theoretical considerations showed that the rate of energy transfer from an energy donor embedded within a membrane to acceptors dissolved in solvent could be described by an analytical function of the distance a of closest approach between the donor and acceptor, if the "rapid-diffusion limit" was attained. The criterion for this limit was given by the relation: (RO)6 much less than 20D tau Da4, where RO is the characteristic distance of energy transfer, D is the diffusion coefficient of the acceptor and tau D is the fluorescence lifetime of the donor in the absence of acceptor. By photo-reduction of the purple membrane with sodium borohydride, the retinal chromophore was converted to a highly fluorescent derivative, which showed a broad emission band in the visible region. From analysis of the fluorescence decay curves of the photo-reduced purple membrane in the presence of various concentrations of cobalt-ethylenediamine tetraacetate (Co-EDTA: energy acceptor), the depth of the chromophore from the membrane surface was estimated to be 8 (+/-3) A. This result was supported by investigations of energy transfer processes in a system where the native purple membranes and the photo-reduced membranes were stacked in parallel: the energy acceptor in this system was the native retinal chromophore.     

Heterodimeric DNA-binding dyes designed for energy transfer: synthesis and spectroscopic properties.

Heterodimeric dyes are described which bind tightly to double-stranded (dsDNA) with large fluorescence enhancements. These dyes are designed to exploit energy transfer between donor and acceptor chromophores to tune the separation between excitation and emission wavelengths. The dyes described here absorb strongly at the 488 nm argon ion line, but emit at different wavelengths, and can be applied to multiplex detection of various targets. The chromophores in these dyes, a thiazole orange-thiazole blue heterodimer (TOTAB), two different thiazole orange-ethidium heterodimers (TOED1 and TOED2), and a fluorescein-ethidium heterodimer (FED), are in each case linked through polymethyleneamine linkers. The emission maxima of the DNA-bound dyes lie at 662 (TOTAB), 614 (TOED 2), and 610 nm (FED). The dyes showed a > 100 fold enhancement of the acceptor chromophore fluorescence on binding to dsDNA and no sequence selectivity. In comparison with direct 488 nm excitation of the constituent monomeric dyes, in the heterodimers the fluorescence of the acceptor chromophores was greatly enhanced and the emission of the donor chromophores quenched by over 90%. The acceptor emission per DNA-bound dye molecule was constant from 100 DNA bp:dye to 20 bp:dye and decreased sharply at higher dye:DNA ratios.     

Distance distributions from the tyrosyl to disulfide residues in the oxytocin and [Arg8]-vasopressin measured using frequency-domain fluorescence resonance energy transfer

We have examined the fluorescence intensity decays of oxytocin and [Arg⁸]-vasopressin resulting from the single tyrosyl residue in each peptide, and the intensity decay of the Asu ^1,6-analogues in which the disulfide bridge is substituted by a CH₂-CH₂ bridge. Viscosity-dependent steady state and intensity decay measurements indicated that fluorescence resonance energy transfer (FRET) from tyrosyl phenol to the disulfide bridge is responsible for the decrease in fluorescence relative to the Asu-analogues. The frequency-domain phase and modulation data for the tyrosyl donor were interpreted in terms of fluorescence resonance energy transfer (FRET) to the weakly absorbing disulfide bridge and a distribution of donor-to-acceptor distances. Energy transfer efficiencies were determined from both time-resolved and steady-state measurements. Fitting the frequency-domain phase and modulation data to a Gaussian distance distribution indicated that the average inter-chromophoric distance (R_av) is similar in both compounds, R_av=7.94 Å for oxytocin and R_av = 8.00 Å for vasopressin. However, the width of the distance distribution is narrower for vasopression (hw =2.80 Å) than for oxytocin (hw =3.58 Å), which is consistent with restriction of the tyrosine phenol motion due to its stacking with the Phe³ side chain of vasopressin. Finally, the recovered distance distribution functions are compared with histograms describing the distance between the chromophores during the course of long, in vacuo, molecular dynamics runs using the computer program CHARMm and the QUANTA 3.0 parameters.Abbreviations AVP [Arg⁸]-vasopressin - FRET fluorescence resonance energy transfer - FD frequency-domain - D donor - A acceptor - DTT dithiothreitol Correspondence to: J. R. Lakowicz     

Simultaneous determination of intramolecular distance distributions and conformational dynamics by global analysis of energy transfer measurements.

Fluorescence energy transfer is widely used for determination of intramolecular distances in macromolecules. The time dependence of the rate of energy transfer is a function of the donor/acceptor distance distribution and fluctuations between the various conformations which may occur during the lifetime of the excited state. Previous attempts to recover both distance distributions and segmental diffusion from time-resolved experiments have been unsuccessful due to the extreme correlation between fitting parameters. A method has been developed, based on global analysis of both donor and acceptor fluorescence decay curves, which overcomes this extreme cross-correlation and allows the parameters of the equilibrium distance distributions and intramolecular diffusion constants to be recovered with high statistical significance and accuracy. Simulation studies of typical intramolecular energy transfer experiments reveal that both static and dynamic conformational distribution information can thus be obtained at a single temperature and viscosity.     

Spatial relationship between the nucleotide-binding site, Lys-61 and Cys-374 in actin and a conformational change induced by myosin subfragment-1 binding

The spatial relationship between Lys-61, the nucleotide binding site and Cys-374 was studied. Lys-61 was labelled with fluorescein-5-isothiocyanate as a resonance energy acceptor, the nucleotide-binding site was labelled with the fluorescent ATP analogues epsilon ATP or formycin-A 5'-triphosphate (FTP) and Cys-374 was labelled with 5-(2-[(iodoacetyl)amino]ethyl)aminonaphthalene-1-sulfonic acid (1,5-IAEDANS) as a resonance energy donor. The distances between the nucleotide binding site and Lys-61 or between Lys-61 and Cys-374 were calculated to be 3.5 +/- 0.3 nm and 4.60 +/- 0.03 nm, respectively. (The assumption has been made in calculating these distances that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime.) On the other hand, when doubly-labelled actin with 1,5-IAEDANS at Cys-374 and FITC at Lys-61 was polymerized in the presence of a twofold molar excess of phalloidin [Miki, M. (1987) Eur. J. Biochem. 164, 229-235], the fluorescence of 1,5-IAEDANS bound to actin was quenched significantly. This could be attributed to inter-monomer energy transfer. The inter-monomer distance between FITC attached to Lys-61 in a monomer and 1,5-IAEDANS attached to Cys-374 in its nearest-neighbour monomer in an F-actin filament was calculated to be 3.34 +/- 0.06 nm, assuming that the likely change in the intra-monomer distance does not change during polymerization by more than 0.4 nm. One possible spatial relationship between Lys-61, Cys-374 and the nucleotide binding site in an F-actin filament is proposed. The effect of myosin subfragment-1 (S1) binding on the energy transfer efficiency was studied. The fluorescence intensity of AEDANS-FITC-actin decreased by 30% upon interaction with S1. The fluorescence intensity of AEDANS-FITC-actin polymer in the presence of phalloidin increased by 21% upon interaction with S1. The addition of ATP led to the fluorescence intensity returning to the initial level. Assuming that the change of fluorescence intensity can be attributed to conformational change in the actin molecule induced by S1 binding, the intra-monomer distance was reduced by 0.4 nm and the inter-monomer distance was increased by 0.2 nm.     

Optimizing the cationic conjugated polymer-sensitized fluorescent signal of dye labeled oligonucleotide for biosensor applications

Methods for real time, highly selective and sensitive polynucleotide detection are of vast scientific and economic importance. Fluorescence resonance energy transfer (FRET)-based assays which take advantage of the collective response of water-soluble conjugated polymers (CPs) and the self-assembly characteristic of aqueous polyelectrolytes have been widely used for the detection of DNA, RNA, protein and small molecules. The detection sensitivity of CP-based biosensor is dependent on the signal amplification of dye emission upon excitation of CP relative to that upon direct excitation of the dye. Using cationic polyfluorene derivatives and chromophore (fluorescein or Texas Red) labeled single-stranded DNA molecules (ssDNA-C*) as donor/acceptor pairs, we show that in addition to the spectral overlap, orientation and distance between the donor and the acceptor, the energy levels and fluorescence quenching of the donor/acceptor within the polymer/DNA-C* complexes are also important factors that affect the signal output of dye emission.     

Molecular dynamics study of chemically engineered green fluorescent protein mutants: comparison of intramolecular fluorescence resonance energy transfer rate

Because of its unusual spectroscopic properties, green fluorescent protein (GFP) has become a useful tool in molecular genetics, biochemistry and cell biology. Here, we computationally characterize the behavior of two GFP constructs, designed as bioprobes for enzymatic triggering using intramolecular fluorescence resonance energy transfer (FRET). These constructs differ in the location of an intramolecular FRET partner, an attached chemical chromophore (either near an N-terminal or C-terminal site). We apply the temperature replica exchange molecular dynamics method to the two flexible constructs in conjunction with a generalized Born implicit solvent model. The calculated rate of FRET was derived from the interchromophore distance, R, and orientational factor, kappa(2). In agreement with experiment, the construct with the C-terminally attached dye was predicted to have higher energy transfer rate than observed for the N-terminal construct. The molecular basis for this observation is discussed. In addition, we find that the orientational factor, kappa(2), deviates from the commonly assumed value, the implications of which are also considered.     

Energy transfer in lipid bilayers.

The quenching of fluorescence due to energy transfer between a dilute, random array of donor and acceptor chromophores in lipid bilayer was measured and compared to theoretical expressions developed to predict the decrease in emission intensity under these circumstances. The observed intensity was found to be the same function of quencher concentration in both planar, multilamellar dispersions and small, spherical vesicles. The degree of quenching was accurately predicted by a simple relation derived in this paper, as well as a more complex equation previously developed by Tweet, et al. The results suggest that significant quenching may be observed even when the average donor-acceptor separation exceeds the F?rster critical distance by severalfold. Application of these results to problems of current interest in membrane research are discussed.     

Orientation factor in steady-state and time-resolved resonance energy transfer measurements.

Resonance energy transfer measurements provide a way to estimate distances between chromophores attached to different sites of macromolecules. There are two unknowns involved in resonance energy transfer measurements, the distance between two chromophores and their relative orientation. When static orientational disorder exists, the orientation factor, kappa 2, can vary from 0 to 4, leading to considerable uncertainty in estimation of distances. Fluorescence polarization anisotropy measurements can reduce the degree of uncertainty [Dale & Eisinger (1974) Biopolymers 13, 1573]. There may still be substantial error bounds for the average distance measurements. Time-resolved fluorescence measurements provide an "apparent" average distance and distance distribution containing contributions by both distance and orientation. The contribution of orientation to observed "apparent" average distance and distance distribution widths has been estimated for both simulated and real data. With a single unique distance as input in the simulation and with random but static orientation of donor and acceptor, the recovered average distance is very close to that of the input when the input distance is close to or larger than the F?rster distance. The recovered width of apparent distance distribution can be substantial and it changes as a function of F?rster distance to average distance ratio and as a function of F?rster distance. Similar conclusions apply to the case where there is a real distance distribution. Motional averaging of the orientation was simulated by the Monte Carlo method to estimate the contribution of orientation when chromophores have certain degrees of mobility.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structural heterogeneity and quantitative FRET efficiency distributions of polyprolines through a hybrid atomistic simulation and Monte Carlo approach

Förster Resonance Energy Transfer (FRET) experiments probe molecular distances via distance dependent energy transfer from an excited donor dye to an acceptor dye. Single molecule experiments not only probe average distances, but also distance distributions or even fluctuations, and thus provide a powerful tool to study biomolecular structure and dynamics. However, the measured energy transfer efficiency depends not only on the distance between the dyes, but also on their mutual orientation, which is typically inaccessible to experiments. Thus, assumptions on the orientation distributions and averages are usually made, limiting the accuracy of the distance distributions extracted from FRET experiments. Here, we demonstrate that by combining single molecule FRET experiments with the mutual dye orientation statistics obtained from Molecular Dynamics (MD) simulations, improved estimates of distances and distributions are obtained. From the simulated time-dependent mutual orientations, FRET efficiencies are calculated and the full statistics of individual photon absorption, energy transfer, and photon emission events is obtained from subsequent Monte Carlo (MC) simulations of the FRET kinetics. All recorded emission events are collected to bursts from which efficiency distributions are calculated in close resemblance to the actual FRET experiment, taking shot noise fully into account. Using polyproline chains with attached Alexa 488 and Alexa 594 dyes as a test system, we demonstrate the feasibility of this approach by direct comparison to experimental data. We identified cis-isomers and different static local environments as sources of the experimentally observed heterogeneity. Reconstructions of distance distributions from experimental data at different levels of theory demonstrate how the respective underlying assumptions and approximations affect the obtained accuracy. Our results show that dye fluctuations obtained from MD simulations, combined with MC single photon kinetics, provide a versatile tool to improve the accuracy of distance distributions that can be extracted from measured single molecule FRET efficiencies.     

Structural information on nanomolecular systems revealed by FRET

Our newly developed fluorescence resonance energy transfer (FRET) based technique, fluorescence nanotomography (FN), is used to determine the morphology and dynamics of some soft materials and bio-molecules by attaching donor (D) fluorophores and acceptors (A) to the investigated structure and using fluorescence lifetime measurements to reveal the D-A distance distribution function rhoDA(r). We report the effect of the limited sizes of the donor and acceptor, effect of porous polymer, and molecular structure and phase transition in phospholipid bilayers.     

Multistep fluorescence resonance energy transfer in sequential chromophore array constructed on oligo-DNA assemblies

Sequential arrays of chromophores at regulated distances were constructed on a noncovalent DNA molecular assembly system in aqueous media. Photoinduced fluorescence resonance energy transfer (FRET) behaviors were then observed. We designed a number of chromophore/oligo-DNA conjugates with varying sequences. The chromophores eosin (Eo), TexasRed (TR), and tetramethylrhodamine (Rho) were employed as the energy donor, acceptor, and mediator, respectively, based on overlapping excitation and emission spectra. The chromophores were attached via aminolinkers to the 5'-terminals of 10mer oligo-DNAs consisting of AT rich sequences. The arrangement of Eo-Rho or Rho-TR with 10-residue (1 pitch of duplex) distances was ensured by duplex formation of the conjugates with a 20mer matrix oligo-DNA composed of complementary sequences to the conjugates. Single-step FRET from Eo to Rho and from Rho to TR was confirmed on the duplex. The three chromophore conjugates were then mixed with longer matrix oligo-DNAs (30 or 40mer) consisting of complementary sequences to the conjugates, producing Eo-(Rho)(n)-TR (n = 1 or 2) arrays with 10-residue distances. Multistep FRET from Eo to TR through the Rho mediator(s) was observed on the molecular assemblies. This photoenergy transmission system offers a good model for a photoenergy transmission system mimicking photosynthetic systems.