Real-time background suppression during frequency domain lifetime measurements

We describe real time background suppression of autofluorescence from biological samples during frequency domain or phase modulation measurements of intensity decays. For these measurements the samples were excited with a train of light pulses with widths below 1 ps. The detector was gated off for a short time period of 10 to 40 ns during and shortly after the excitation pulse. The reference signal needed for the frequency domain measurement was provided by a long-lifetime reference fluorophore which continues to emit following the off-gating pulse. Both the sample and the reference were measured under identical optical and electronic conditions avoiding the need for correction of the photomultiplier tube signal for the gating sequence. We demonstrate frequency domain background suppression using a mixture of short- and long-lifetime probes and for a long-lifetime probe in human plasma with significant autofluorescence.     

Time-gated in vivo autofluorescence imaging of dental caries.

Laser-induced time-resolved autofluorescence from carious lesions of human teeth was studied by means of ultrashort pulsed laser systems, time-correlated single photon counting and time-gated imaging. Carious regions exhibited a slower fluorescence decay with a main 17 ns fluorescence lifetime than healthy hard dental tissue. The long-lived fluorophore present in carious lesions only emits in the red spectral region. Fluorescence decay time and spectral characteristics are typical of fluorescent metal-free porphyrin monomers. The spatial distribution of the long-lived endogenous porphyrin fluorophore within the tooth material was detected by time-gated nanosecond autofluorescence imaging. In particular, high contrast video images were obtained with an appropriate time delay of 15 ns to 25 ns between excitation and detection due to the suppression of short-lived autofluorescence of healthy tissue. First in vivo applications are reported indicating the potential of time-resolved fluorescence diagnostics for early caries- and dental plaque detection.     

Subtraction of background fluorescence in multiharmonic frequency-domain fluorimetry.

Background fluorescence is a major concern in time-resolved microfluorimetry studies of biological samples. A general method for subtraction of an arbitrary background signal in measurements of lifetime and anisotropy decay by multiharmonic Fourier transform spectroscopy is presented. Multifrequency phase and modulation values are measured in parallel by transformation of digitized time-domain waveforms into the frequency domain. For subtraction of background, time-domain waveforms are acquired for emission and reference photomultipliers for sample (e.g., cell containing fluorophore) and blank (e.g., unlabeled cell). Time-domain waveforms obtained in a series of measurements (e.g., sample and blank for parallel and perpendicular orientations of an emission polarizer) are time-justified by least-squares fitting of reference channel waveforms or by phase comparison of the first Fourier harmonics of the reference channel. Background is then subtracted directly in the time domain, and the subtracted waveform is Fourier transformed to the frequency domain for analysis of lifetime or anisotropy decay. This approach yielded excellent background correction over a wide range of background intensities and decay profiles. The method was tested in cuvette fluorimetry with fluorescein and acridine orange and in fluorescence microscopy with living MDCK cells loaded with the pH indicator BCECF. Sample lifetimes and rotational parameters could be recovered accurately with greater than 50% of the signal arising from background. These results establish a direct and practical approach to subtraction of background in complex biological and chemical samples studied by frequency-domain fluorimetry.     

Fluorescence lifetime optical projection tomography

We describe a quantitative fluorescence projection tomography technique which measures the 3‐D fluorescence lifetime distribution in optically cleared specimens up 1 cm in diameter. This is achieved by acquiring a series of wide‐field time‐gated images at different relative time delays with respect to a train of excitation pulses, at a number of projection angles. For each time delay, the 3‐D time‐gated intensity distribution is reconstructed using a filtered back projection algorithm and the fluorescence lifetime subsequently determined for each reconstructed horizontal plane by iterative fitting to a mono‐exponential decay. Due to its inherently ratiometric nature, fluorescence lifetime is robust against intensity based artefacts as well as producing a quantitative measure of the fluorescence signal. We present a 3‐D fluorescence lifetime reconstruction of a mouse embryo labelled with an alexa‐488 conjugated antibody targeted to the neurofilament, which clearly differentiates between the extrinsic label and the autofluorescence, particularly from the heart and dorsal aorta. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Picosecond resolution of tyrosine fluorescence and anisotropy decays by 2-GHz frequency-domain fluorometry

We extended the technique of frequency-domain fluorometry to an upper frequency limit of 2000 MHz. This was accomplished by using the harmonic content of a laser pulse train (3.76 MHz, 5 ps) from a synchronously pumped and cavity-dumped dye laser. We used a microchannel plate photomultiplier as the detector to obtain the 2-GHz bandwidth. This new instrument was used to examine tyrosine intensity and anisotropy decays from peptides and proteins. These initial data sets demonstrate that triply exponential tyrosine intensity decays are easily recoverable, even if the mean decay time is less than 1 ns. Importantly, the extended frequency range provides good resolution of rapid and/or multiexponential tyrosine anisotropy decays. Correlation times as short as 15 ps have been recovered for indole, with an uncertainty of +/- 3 ps. We recovered a doubly exponential anisotropy decay of oxytoxin (29 and 454 ps), which probably reflects torsional motions of the phenol ring and overall rotational diffusion, respectively. Also, a 40-ps component was found in the anisotropy decay of bovine pancreatic trypsin inhibitor, which may be due to rapid torsional motions of the tyrosine residues and/or energy transfer among these residues. The rapid component has an amplitude of 0.05, which is about 16% of the total anisotropy. The availability of 2-GHz frequency-domain data extends the measurable time scale for fluorescence to overlap with that of molecular dynamics calculations.     

Correction for contaminant fluorescence in frequency-domain fluorometry

We describe a general method to correct for contaminant fluorescence when using the technique of frequency-domain fluorometry. The method can be applied regardless of the origin of the background signal, from scattered light, impurity fluorescence, or both. The procedure requires measurement of the frequency-dependent phase and modulation of the background at enough frequencies to approximate the decay law of the background. We also describe a general method to propagate the uncertainties in the measured phase and modulation values into the corrected values. This propagation is necessary to ensure proper weighting of the frequency-dependent data in the least-squares fitting algorithms. The practical usefulness of this correction method is demonstrated using frequency-domain data for one and two component mixtures which were deliberately contaminated with scattered light and/or other fluorophores.     

Demonstration of an associated anisotropy decay by frequency-domain fluorometry

We used frequency-domain fluorometry to demonstrate the presence of an associated decay of fluorescence anisotropy. In such systems the individual correlation times are associated with distinct emitting species, each with its own characteristic lifetime and rotational correlation times. We obtained an associated system using 1-anilino-8-naphthalenesulfonic acid (ANS) in the presence of increasing amounts of apomyoglobin. When both free and apomyoglobin-bound ANS contributed to the emission the differential polarized phase angles become negative at particular frequencies, even though the fundamental anisotropy (r0) is greater than zero. Additionally, the modulated anisotropy decreases at high frequencies. Both observations appear to be the unique consequence of an associated anisotropy decay, and are not possible for a multiexponential anisotropy decay of a single species.     

Correction of timing errors in photomultiplier tubes used in phase-modulation fluorometry

The measurement of fluorescence lifetimes is known to be hindered by the wavelenght-dependent and photocathode area-dependent time response of photomultiplier tubes. A simple and direct method is described to minimize the effects in photomultiplier tubes for phase-modulation fluorometry. Reference fluorophores of known lifetime were used in place of the usual scattering reference. The emission wavelenghts of the reference and sample were matched by either filters or a monochromator, and the use of a fluorophore rather than a scatter decreases the differences in spatial distribution of light emanating from the reference and sample. Thus photomultiplier tube artifacts are minimized. Five reference fluorophores were selected on the basis of availability, ease of solution preparation, and constancy of lifetime with temperature and emission wavelenght. These compounds are p-terphenyl, PPO, PPD, POPOP and dimethyl POPOP. These compounds are dissolved in ethanol to give standard solutions that can be used over the temperature range from ?55 to +55°C. Purging with inert gas is not necessary. The measured phase and modulation of the reference solution is used, in conjunction with the known reference, lifetime, to calculate the actual phase and modulation of the exictation beam. The use of standard fluorophores does not require separate experiments to quantify photomultiplier effects, and does not increase the time required for the measurement of fluorescence lifetimes. Examples are presented which demonstrate the elimination of artifactual photomultiplier effects in measurements of the lifetimes of DADH (0.4 ns) and indole solutions quenched by iodide. In addition, the use of these reference solutions increases the accuracy of fluorescence lifetime measurements ranging ranging to 30 ns. We judge this method to provide more reliable lifetime measurements by the phase and modulation method. The test solutions and procedures we describe may be used by other laboratories to evaluate the performance of their phase fluorometers.     

Comparison of approaches to the instrumental response function in fluorescence decay measurements

Deconvolution of pulse fluorometry data requires knowledge of the instrumental response, which is not directly observable in some circumstances. Various procedures for approaching the instrumental response function were evaluated for nanosecond fluorescence decay data analyzed by nonlinear least squares, including the commonly used time shift correction and several reference fluorophore methods. A new reference fluorophore technique using a Monte Carlo convolution is introduced and tested. The correction for scattered light in several reference techniques is also presented. The random convolution and one other reference fluorophore method consistently gave superior results over a wide range of experimental conditions.     

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.     

Construction and performance of a variable-frequency phase-modulation fluorometer

We describe the construction and performance of a variable-frequency phase-modulation fluorometer. This instrument, which provides modulation frequencies from 1 to 200 MHz, was constructed using commercially available components. To facilitate the introduction of these instruments into other laboratories we describe in detail the chosen components and the principles of operation. The present light source is a continuous-wave helium-cadmium laser, which provides convenient excitation wavelengths of 325 and 442 nm. Modulation of the incident light is provided by one of several electro-optic modulators. The extent of modulation ranges from 1.0 to 0.2 as the frequency increases from 1 to 200 MHz. Phase angles and demodulation factors are measured using the cross-correlation method. The closely spaced frequencies are provided by two direct frequency synthesizers. The phase and modulation measurements are accurate to 0.2 degrees and 0.002, respectively, from 1 to 200 MHz. This accuracy allows considerable resolution of complex decay laws. The usefulness of frequency-domain fluorometry for the resolution of multiexponential decays is illustrated by the analysis of several difficult mixtures. As examples, we resolved a two-component mixture of anthracene (4.1 ns) and 9,10-diphenylanthracene (6.3 ns), and confirmed that the intensity decay of NADH in aqueous buffer is at least a double exponential (0.2 and 0.86 ns). We also resolved an especially difficult mixture of anthracene (4.1 ns) and 9-methylanthracene (4.5 ns), and a three-component mixture with decay times of 1.3, 4.1 and 7.7 ns. Frequency-domain fluorometers appear to be particularly useful for determination of complex decays of fluorescence anisotropy. This capability is illustrated by the determination of rotational correlation times as short as 47 ps for p-bis[2-(5-phenyloxazolyl)]benzene (POPOP) in hexane at 40 degrees C, and by the resolution of the two correlation times of anisotropic rotators such as perylene and 9-aminoacridine. Resolution of two anisotropy decay times for 9-aminoacridine is a difficult test because these correlation times differ by less than 2-fold. The resolution of multiexponential decays of intensity and anisotropy possible with this instrument is at least equivalent to that obtained using state-of-the-art time-resolved instruments based on mode-locked laser sources. The ease and rapidity of frequency-domain measurements, the relative simplicity of the equipment, the accuracy of the measurements and the lack of significant systematic errors indicate that frequency-domain fluorometry will be widely useful in chemical and biochemical research.     

Frequency-domain measurements of the rotational dynamics of the tyrosine groups of calmodulin

We used frequency-domain fluorometry to determine the intensity and anisotropy decay kinetics of tyrosine residues in calmodulin and its fragments. Excitation was provided by a continuous ultraviolet laser source, a frequency-doubled rhodamine 6G ring dye laser, whose output was externally modulated to 200 MHz. Both the intensity and anisotropy decays were found to be multiexponential and dependent upon temperature and solution conditions. By examination of calmodulin fragments we determined that energy transfer between the two tyrosine residues reduces the steady-state anisotropy values by about 20%. Additionally, the frequency-domain anisotropy decays indicate local torsional motions of the tyrosine residues, as well as significant individual motions of the two domains of calmodulin.     

Time-resolved fluorescence of erythrocyte plasma membrane Ca2(+)-ATPase in different functional states.

The fluorescence decay of the plasma membrane calmodulin-activated Ca2(+)-ATPase from the erythrocyte was measured for the first time. The availability of a novel procedure for on-line blank subtraction in frequency-domain lifetime data acquisition (G.G. Reinhart, B. Feddersen, D. Jameson and E. Gratton, Biophys. J. 57 (1990) 189a) permitted the elimination of background interference from detergent-solubilized purified plasma membrane ATPase samples. The fluorescence decay of the erythrocyte Ca2(+)-ATPase was measured in the absence of Ca2+, or in the presence of Ca2+ or Ca2+ plus calmodulin. In the three different experimental conditions the fluorescence decay was very heterogeneous and could be best described by Lorentzian distributions of lifetime values. In the absence of Ca2+ the decay was described by a broad lifetime distribution centered at 4.4 ns with a width of 3.2 ns, indicating heterogeneity of tryptophan microenvironments in the ATPase. Calcium ion binding promoted an 11% increase in the center and a 27% decrease in the width of the distribution. By contrast, addition of calmodulin in the presence of Ca2+ caused a 15% decrease in the center of the distribution, revealing structural difference between calmodulin-activated and Ca2(+)-activated states of the ATPase. These results indicate the usefulness of on-line blank subtraction in frequency-domain lifetime measurements to investigate conformational changes in detergent-solubilized membrane protein samples.     

Lateral diffusion coefficients in membranes measured by resonance energy transfer and a new algorithm for diffusion in two dimensions

We describe measurements of lateral diffusion in membranes using resonance energy transfer. The donor was a rhenium (Re) metal-ligand complex lipid, which displays a donor decay time near 3 micros. The long donor lifetime resulted in an ability to measure lateral diffusion coefficient below 10(-8) cm(2)/s. The donor decay data were analyzed using a new numerical algorithm for calculation of resonance energy transfer for donors and acceptors randomly distributed in two dimensions. An analytical solution to the diffusion equation in two dimensions is not known, so the equation was solved by the relaxation method in Laplace space. This algorithm allows the donor decay in the absence of energy transfer to be multiexponential. The simulations show that mutual lateral diffusion coefficients of the donor and acceptor on the order of 10(-8) cm(2)/s are readily recovered from the frequency-domain data with donor decay times on the microsecond timescale. Importantly, the lateral diffusion coefficients and acceptor concentrations can be recovered independently despite correlation between these parameters. This algorithm was tested and verified using the donor decays of a long lifetime rhenium lipid donor and a Texas red-lipid acceptor. Lateral diffusion coefficients ranged from 4.4 x 10(-9) cm(2)/s in 1,2-dimyristoyl-sn-glycero-3-[phospho-rac-(1-glycerol)] (DMPG) at 10 degrees C to 1.7 x 10(-7) cm(2)/s in 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC) at 35 degrees C. These results demonstrated the possibility of direct measurements of lateral diffusion coefficients using microsecond decay time luminophores.     

Lifetime distributions and anisotropy decays of indole fluorescence in cyclohexane/ethanol mixtures by frequency-domain fluorometry

We used frequency-domain fluorometry to measure intensity and anisotropy decay of indole fluorescence in cyclohexane/ethanol mixtures at 20 degrees C. In 100% cyclohexane or 100% ethanol the intensity decay of indole appears to be a single exponential with decay times of 7.66 and 4.10 ns, respectively. In cyclohexane containing a small percentage of ethanol (up to 10%), we observed increased heterogeneity in intensity decay, resulting in a 10-fold increase in chi 2R for the single-exponential fit, as compared with the double-exponential model. We obtained comparable or better fits using unimodal Lorentzian and Gaussian lifetime distributions (two floating parameters) than for the two-exponential model (three floating parameters). We believe that the distribution of decay times reflects a range of indole solvation states in the dominately nonpolar solutions. This result suggests that a variety of hydrogen-bonding configurations could be one origin of the distributions of decay times observed for tryptophan emission from proteins. We also measured rotational diffusion of indole in cyclohexane, ethanol and its mixtures at 20 degrees C. The picosecond correlation times required that the mean decay times be decreased by acrylamide quenching (in ethanol) or energy transfer (in cyclohexane). In ethanol we observed nearly isotropic rotation of indole; in cyclohexane we obtained two correlation times of 17 and 73 ps. The shorter correlation time in cyclohexane appears to be due to the slip boundary condition, which was found to be progressively eliminated by small percentages of ethanol. Hence, hydrogen-bonding interactions appear to have a substantial effect on the rotational dynamics of indole.     

Measurement of subnanosecond anisotropy decays of protein fluorescence using frequency-domain fluorometry

We report the first anisotropy decays of protein fluorescence obtained using a frequency-domain fluorometer. The ultraviolet light source (300 nm) was a ring dye laser equipped with an intracavity frequency doubler, pumped by an argon ion laser. The data, measured at modulation frequencies from 2 to 200 MHz, reveal the presence of subnanosecond motions (0.1-0.2 ns) of the single tryptophan residues in melittin and monellin. For melittin the data also indicate the presence of slower motions near 1 ns, which may be the result of concerted motions of several peptide units. Smaller amplitude motions, on a similar timescale, were observed for the single tryptophan residue in staphylococcal nuclease. We demonstrate using N-acetyl-L-tryptophanamide in water that the method of frequency-domain fluorometry is capable of measuring correlation times as short as 50 ps. This method can provide data for the direct comparison of measured anisotropy decays with those predicted from molecular dynamics calculations.     

Resolution of the conformational distribution and dynamics of a flexible molecule using frequency-domain fluorometry

We report the first resolution of both the conformational distribution and end-to-end diffusion coefficient of a flexible molecule. This molecular information was recovered using only the donor intensity decay in a single solvent at a single viscosity, as observed by the technique of frequency-domain fluorometry. This technique can be extended to measurements of structural fluctuations of biological macromolecules.     

Detection of phospholipid phase separation. A multifrequency phase fluorimetry study of 1,6-diphenyl-1,3,5-hexatriene fluorescence

Using multifrequency phase and modulation fluorometry and a nonlinear least-squares analysis of lifetime data, we were able to determine the complex decay of 1,6-diphenyl-1,3,5-hexatriene (DPH) in synthetic phospholipid bilayers. Our results showed a monoexponential decay of DPH in the pure isotropic solvents studied, over a wide temperature range, and a double-exponential decay of DPH in phospholipids, both above and below the transition. During the transition, and in mixed-phase phospholipids, a three-component analysis was successfully accomplished, and the pre-exponential factors of the two main components have been shown to be quantitatively representative of the gel and liquid-crystalline phases of the bilayer. The fractional intensity of the shorter lifetime component depends on the modalities of the sample preparation. The factors affecting this component are discussed. From the DPH fluorescence lifetime and from the anisotropy data in L-alpha-dimyristoyl-phosphatidylcholine/L-alpha-dipalmitoyl-phosphatidyl choline mixtures, a phase diagram was independently constructed. Conclusions about the sensitivity and the partition of the probe between gel and the liquid-crystalline phases of the bilayer are derived. Lifetime experiments on DPH in a L-alpha-dilauroyl-phosphatidylcholine/L-alpha-dipalmitoyl-phosphatidylch oline mixture suggested a general method for the determination and quantitation of the two different phases in the bilayer.     

A study of protein dynamics from anisotropy decays obtained by variable frequency phase-modulation fluorometry: internal motions of N-methylanthraniloyl melittin

Internal motions of melittin and its lipid complexes were studied by anisotropy decays determined by frequency-domain fluorometry. A covalent anthraniloyl probe was attached, probably to lysine-21. The emission spectra indicate that the anthraniloyl moiety is exposed to solvent in both monomeric and tetrameric forms and is present at the lipid-water interfacial region in the lipid complexes. The fluorescence intensity decay of melittin in solution and its lipid complexes was characterized by three lifetimes. The lifetimes were near 1-2 ns, 6-7 ns and 10 ns. At increased temperatures there was an increase in the amplitude of the intermediate lifetime and a decrease in that of the longer lifetime. For all the melittin systems, at least three correlation times were required to fit the anisotropy data. Of the three correlation times, the shortest correlation time represents the local motions of the probe, while the longest represents global motions of the whole molecule. The intermediate correlation time probably represents the dynamics of domains/helices within the molecule. The melittin monomer is highly flexible, with greater than 90% of its anisotropy being lost by the local motions. Even though it is well organized (greater than 75% helical), the tetramer is still a highly flexible molecule, with 70% of its anisotropy being lost by the local motions. The internal motions of melittin decrease upon binding to lipids and are sensitive to the phase state of the lipid complexes.