Three-photon induced fluorescence of the calcium probe Indo-1.

We report the calcium-dependent emission spectral properties of the calcium probe Indo-1 for three-photon excitation. We found that Indo-1 could be readily excited with the femtosecond pulses from a mode-locked Ti:sapphire laser at 885 nm. This wavelength is too long for two-photon excitation, which is expected to occur for wavelengths no longer than twice the longest single-photon absorption wavelength of 400 nm. For excitation at 885 nm the emission intensity was found to depend on the cube of the laser power, as expected for simultaneous interaction with three photons. At wavelengths below 840 nm the emission intensity depends on the square of the laser power, indicating two-photon excitation at shorter wavelengths. The intensity decays of Indo-1 were found to be dependent on Ca2+ and essentially identical for one- and three-photon excitation. The emission anisotropy of Indo-1 was found to be considerably higher for three-photon excitation than for one-photon excitation, consistent with cos6 theta photoselection, as compared with cos2 theta photoselection for one-photon excitation. The high values of the anisotropy are in agreement with those expected for a three-photon process. Calcium-dependent emission spectra were observed for Indo-1 with three-photon excitation, demonstrating that three-photon excitation of Indo-1 can be used for calcium imaging by emission intensity ratio measurements. The calcium-dependent emission spectra indicate a higher three-photon cross-section for the calcium-free form of Indo-1 than for the calcium-bound form. The possible advantages of three-photon excitation include the availability of the appropriate wavelengths with solid-state lasers, enhanced spatial resolution due to a reduced size of the excited volume, absence of light quenching, and possibly high selectivity of the three-photon excitation process.     

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.     

Three-photon excitation of N-acetyl-L-tyrosinamide.

We observed emission from the tyrosine derivative N-acetyl-L-tyrosinamide (NATyrA) when excited with the fundamental output of a femtosecond Ti:Sapphire laser from 780 to 855 nm. The dependence on incident laser power indicates a three-photon process. The emission spectra and intensity decay in glycerol-water (30:70) at 5 degrees C were found to be identical for one- and three-photon excitation. Also the excitation spectrum of three-photon-induced fluorescence of NATyrA corresponds to the one-photon excitation spectrum. The time-zero or fundamental anisotropy spectrum was reconstructed from the frequency-domain anisotropy decays. The three-photon anisotropies are similar or larger than the one-photon anisotropies. These three-photon anisotropies are surprising given the near zero values known for tyrosine with two-photon excitation. The observations indicate that one- and three-photon excitation directly populates the same singlet excited states(s). However, the origin of the anisotropies with multi-photon excitation of tyrosine remain unclear and unpredictable.     

Fluorescence spectral properties of troponin C mutant F22W with one-, two-, and three-photon excitation.

We report the first measurements of protein fluorescence with three-photon excitation, using a mutant of troponin C (TnC) that contains a single tryptophan residue F22W. From the emission intensity dependence on laser power we determine that TnC F22W displays one-, two-, and three-photon excitation at 285, 570, and 855 nm, respectively. The emission spectra and intensity decays are identical for one-, two-, or three-photon excitation. The steady-state and time 0 anisotropies are distinct for each mode of excitation, but the correlation times were the same, suggesting that three-photon excitation of proteins can be accomplished without significant effects of the locally intense illumination. The excitation anisotropy spectrum from 830 to 900 nm displays only negative values, suggesting dominant excitation via the 1Lb state of tryptophan from 830 to 900 nm.     

Time-resolved spectral observations of cadmium-enriched cadmium sulfide nanoparticles and the effects of DNA oligomer binding

We measured the steady-state and time-resolved fluorescence spectral properties of cadmium-enriched nanoparticles (CdS-Cd2+). These particles displayed two emission maxima, at 460 and 580 nm. The emission spectra were independent of excitation wavelength. Surprisingly, the intensity decays were strongly dependent on the observation wavelength, with longer decay times being observed at longer wavelengths. The mean lifetime increased from 150 to 370 ns as the emission wavelength was increased from 460 to 650 nm. The wavelength-dependent lifetimes were used to construct the time-resolved emission spectra, which showed a growth of the long-wavelength emission at longer times, and decay-associated spectra, which showed the longer wavelength emission associated with the longer decay time. These nanoparticles displayed anisotropy values as high as 0.35, depending on the excitation and emission wavelengths. Such high anisotropies are unexpected for presumably spherical nanoparticles. The anisotropy decayed with two correlation times near 5 and 370 ns, with the larger value probably due to overall rotational diffusion of the nanoparticles. Addition of a 32-base pair oligomer selectively quenched the 460-nm emission, with less quenching being observed at longer wavelengths. The time-resolved intensity decays were minimally affected by the DNA, suggesting a static quenching mechanism. The wavelength-selected quenching shown by the nanoparticles may make them useful for DNA analysis.     

Characterization of the tryptophan fluorescence from sarcoplasmic reticulum adenosinetriphosphatase by frequency-domain fluorescence spectroscopy

We examined the tryptophan decay kinetics of sarcoplasmic reticulum Ca2+-ATPase using frequency-domain fluorescence. Consistent with earlier reports on steady-state fluorescence intensity, our intensity decays reveal a reproducible and statistically significant 2% increase in the mean decay time due to calcium binding to specific sites involved in enzyme activation. This Ca2+ effect could not be eliminated with acrylamide quenching, which suggests a global effect of calcium on the Ca2+-ATPase, as opposed to a specific effect on a single water-accessible tryptophan residue. The tryptophan anisotropy decays indicate substantial rapid loss of anisotropy, which can be the result of either intramolecular energy transfer or a change in segmental flexibility of the ATPase protein. Energy transfer from tryptophan to TNP-ATP in the nucleotide binding domain, or to IEADANS on Cys-670 and -674, indicates that most tryptophan residues are 30 A or further away from these sites and that this distance is not decreased by Ca2+. In light of known structural features of the Ca2+-ATPase, the tryptophan fluorescence changes are attributed to stabilization of clustered transmembrane helices resulting from calcium binding.     

Nanosecond fluorescence microscopy. Emission kinetics of fura-2 in single cells.

A microscope based time-correlated single photon counting instrument has been constructed to measure fluorescence intensity and emission anisotropy decays from fluorophores in single cells on a nanosecond time scale. The sample is excited and the emission collected using epi-illumination optics with frequency-doubled pulses from the cavity-dumped output of a synchronously pumped dye laser serving as an excitation source. Collection of decays from a single cell is possible due to the presence of an iris in the emission path that can be reduced to less than the diameter of a single cell. Using the instrument the decay of 60 nM 1,6-diphenyl-1,3,5-hexatriene was measured, demonstrating that adequate data for lifetime analysis can be recorded from fewer 10(3) molecules of the fluorophore in an illuminated volume of 23 fl. In addition, the intensity and anisotropy decays of fura-2 in single adherent cells and in suspensions of fura-2 loaded cells in suspension, although the relative amplitudes and decay constants vary somewhat from cell to cell. The results indicate that a significant but variable fraction of fura-2 is bound to relatively immobile macromolecular components in these cells.     

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.     

Anisotropy decays of indole, melittin monomer and melittin tetramer by frequency-domain fluorometry and multi-wavelength global analysis

We used frequency-domain fluorescence spectroscopy to measure the fluorescence lifetime and anisotropy decays of indole in propylene glycol, and of the tryptophan emission of melittin monomer and tetramer in water solutions at 5 degrees C. We obtained an increase in resolution of the anisotropy decays by using multiple excitation wavelengths, chosen to provide a range of fundamental anisotropy values. The multi-excitation wavelength anisotropy decays were analyzed globally to recover a single set of correlation times with wavelength-dependent anisotropy amplitudes. Simulated data and kappaR2 surfaces are shown to reveal the effect of multi-wavelength data on the resolution of complex anisotropy decays. For both indole and melittin, the anisotropy decays are heterogeneous and require two correlation times to fit the frequency-domain data. For indole in propylene glycol at 5 degrees C we recovered correlation times of 0.59 and 4.10 ns, which appear to be characteristic of the rigid and asymmetric indole molecule. For melittin monomer the correlation times were 0.13 and 1.75 ns, and for melittin tetramer 0.12 and 3.96 ns. The shorter and longer correlation times of melittin are due to segmental motions and overall rotational diffusion of the polypeptide.     

On the effect of sodium dodecyl sulfate on the structure of beta-galactosidase from Escherichia coli. A fluorescence study.

An understanding of the structure-function relationship of proteins under different chemical-physical conditions is of fundamental importance for an understanding of their structure and function in cells. In this paper we report the effects of sodium dodecyl sulfate and temperature on the structure of beta-galactosidase from Escherichia coli, as monitored by fluorescence spectroscopy. The structure of the protein was studied in the temperature range of 10-60 degrees C in the absence and presence of sodium dodecyl sulfate by frequency-domain measurement of the intrinsic fluorescence intensity and anisotropy decays. The time-resolved fluorescence data in the absence of SDS indicated that at 10 degrees C the tryptophanyl emission decays were well described by a three exponential decays model, and that the temperature increase resulted in shortening of the long-lived component with little change in the short- and middle-lived components. The addition of SDS to the protein solution also affected the long-lived component. The effects of the detergent and temperature on the enzyme structure were also investigated by means of quenching experiments and anisotropy decays. The obtained results showed that the presence of SDS confers more flexibility to the protein structure, and suggest a strict relation between enzyme activity and protein flexibility.     

Diffusion coefficients of quenchers in proteins from transient effects in the intensity decays

We used 2-GHz frequency-domain fluorometry to examine the intensity decays of N-acetyl-L-tryptophamide (NATA) and the protein staphylococcal nuclease in the presence and absence of quenching by oxygen or acrylamide. When analyzed with a multiexponential model, the decays of NATA and nuclease both become more heterogeneous in the presence of quenching. We attribute the increased complexity to transient effects in quenching or equivalently a time-dependent rate constant for quenching. The frequency-domain data were analyzed using the Smoluchowski model (exp(-t/tau-2b square root t)) and the radiation model, which is known to correct some flaws in the more approximate Smoluchowski model. The radiation model provides improved fits to the data, as evidenced by average 10-fold decreases in chi R2. The radiation model also provides an estimate of the sum of the diffusion coefficients and the specific rate constant for quenching. The apparent diffusion coefficients for acrylamide and oxygen in nuclease, as seen by its single tryptophan (residue 140) are 15- and 11-fold lower than in water, respectively. The apparent values of the oxygen diffusion coefficient in water, as seen by NATA, are 2- to 3-fold larger than expected from earlier steady-state measurements. The ability to recover the detailed form of the intensity decays by the frequency-domain method should allow comparison of experimental results with calculated trajectories of quenchers in proteins.     

Tryptophan fluorescence intensity and anisotropy decays of human serum albumin resulting from one-photon and two-photon excitation.

We measured the emission spectra, intensity decays and anisotropy decays of the single tryptophan residue of human serum albumin (HSA) resulting from one-photon (295-298 nm) and two-photon (590-596) excitation. The emission spectra and intensity decays were independent of the mode of excitation. The anisotropy decays were superficially similar for one- and two-photon excitation. However, upon consideration of the different orientation photoselection for one- and two-photon excitation, the anisotropy data reveal different angles between the absorption and emission oscillators for one-photon and two-photon excitation. This result suggests different relative one-photon and two-photon cross-sections for the 1La and 1Lb transitions of the indole residue. This first report of the time-resolved anisotropy decay of a protein resulting from two-photon excitation suggests that such measurement will yield insights into the complex photophysical properties of tryptophan residues in proteins.     

Exciton Annihilation in the Two Photosystems in Chloroplasts at 100°K

The fluorescence yield (F) of spinach chloroplasts at 100°K measured at 735 nm (photosystem I fluorescence—F 735) and at 685 nm (photosystem II fluorescence—F 685) has been determined with different modes of laser excitation. The modes of excitation included a single picosecond pulse, sequences of picosecond pulses (4, 22, and 300 pulses spaced 5 ns apart) and a single nonmode-locked 2-μs pulse (MP mode). The F 735/F 685 intensity ratios decrease from 1.62 to 0.61 when a single picosecond pulse (or low-power continuous helium-neon laser) is replaced by excitation with the 300-ps pulse train (PPT mode) or MP mode. In the PPT mode of excitation, the 735-nm fluorescence band is quenched by a factor of 45 as the intensity is increased from 10¹⁵ to 10¹⁸ photons/cm² per pulse train and the 685-nm fluorescence is quenched by a factor of 10. In the MP mode, the quenching factors are 25 and 7, respectively, in the same intensity range. Fluorescence quantum yield measurements with different picosecond pulse sequences indicate that relatively long-lived quenching species are operative, which survive from one picosecond pulse to another within the pulse train. The excitonic processes possible in the photosynthetic units are discussed in detail. The differences in the quenching factors between the MP and PPT modes of excitation are attributed to singlet-singlet annihilation, possible when picosecond pulses are utilized, but minimized in the MP mode of excitation. The long-lived quenchers are identified as triplets and/or bulk chlorophyll ions formed by singlet-singlet annihilation. The preferential quenching in photosystem I is attributed to triplet excitons. The influence of heating effects, photochemistry, bleaching, and two-photon processes is also considered and is shown to be negligible.     

Picosecond resolution of oxytocin tyrosyl fluorescence by 2 GHz frequency-domain fluorometry

The technique of frequency-domain fluorometry has been extended to 2000 MHz using the harmonic content of a picosecond laser source and a microchannel plate photomultiplier tube. This new instrument was used to resolve complex subnanosecond intensity and anisotropy decays of the tyrosyl emission of oxytocin. The intensity decay was found to contain at least three exponential components, 80, 359 and 927 ps. The anisotropy analysis revealed a 29 ps torsional motion of the tyrosine residue as well as a 454 ps overall rotational correlation time. The time resolution of this method should permit the comparison of experimental results with theoretical models for motions of proteins.     

Conformation and dynamics of bovine brain S-100a protein determined by fluorescence spectroscopy.

We have used time-resolved laser fluorescence spectroscopy to investigate the intensity and anisotropy decays of the single tryptophan residue in bovine brain S-100a (alpha beta) protein. The steady-state and acrylamide quenching results indicated that the Trp 90 of the alpha-subunit was partially buried in a relatively nonpolar environment at pH 7.5. Both Ca2+ and pH 8.5 slightly enhanced the exposure of the residue to the solvent, but the residue remained partially buried in the calcium complex at both pH values. The best representation of the intensity decays was a linear combination of three exponential terms, regardless of solvent condition and temperature. The three lifetimes (tau i) were in the range of 0.4-5 ns and insensitive to emission wavelength, but their fractional amplitudes (alpha i) shifted in favor of the shortest component (alpha 1) when the decays were measured at the blue end of the emission spectrum. These results suggest that an excited-state interaction between the indole ring and the side chain of an adjacent residue may be responsible for the observed shortest lifetime. In the presence of Ca2+, the three lifetimes remained relatively unaltered, but the values of alpha 1 decreased by a factor of 2.3 at pH 7.2 and a factor of 1.8 at pH 8.2. This Ca(2+)-induced decrease may be attributed to disruption of the putative excited-state interaction resulting from reorientations of the alpha-helical segments flanking a Ca(2+)-binding loop (residues 62-73). At both pH 7.2 and 8.4, the anisotropy decays of the apoprotein followed a biexponential decay law.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Theory of photoselection by intense light pulses. Influence of reorientational dynamics and chemical kinetics on absorbance measurements.

The theory of absorbance measurements on a system (e.g., chromophore(s) in a protein) that undergoes a sequence of reactions initiated by a linearly polarized light pulse is developed for excitation pulses of arbitrary intensity. This formalism is based on a set of master equations describing the time evolution of the orientational distribution function of the various species resulting from excitation, reorientational dynamics, and chemical kinetics. For intense but short excitation pulses, the changes in absorbance (for arbitrary polarization directions of the excitation and probe pulses) and the absorption anisotropy are expressed in terms of reorientational correlation functions. The influence of the internal motions of the chromophore as well as the overall motions of the molecules is considered. When the duration of the excitation pulse is long compared to the time-scale of internal motions but comparable to the overall correlation time of the molecule that is reorienting isotropically, the problem of calculating the changes in absorbance is reduced to the solution of a set of first-order coupled differential equations. Emphasis is placed on obtaining explicit results for quantities that are measured in photolysis and fluorescence experiments so as to facilitate the analysis of experimental data.     

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.     

Global analysis of steady-state polarized fluorescence spectra using trilinear curve resolution.

Global analysis using trilinear curve resolution is described and shown to be a powerful method for the resolution of polarized fluorescence data arrays, in which the measured fluorescence intensity is a separable function of polarization orientation, excitation wavelength, and emission wavelength. This methodology is applicable to mixtures the components of which have linearly independent excitation and emission spectra and distinct anisotropies. Normalized excitation and emission spectra of individual components can be uniquely determined without prior assumptions concerning spectral shapes (e.g., sum of Gaussians) and without the uncertainties inherent in bilinear techniques such as principal component analysis or factor analysis. The normalized excitation and emission vectors are combined with the total absorption spectrum of the multicomponent mixture to compute absolute absorption and emission spectra. The precision of this methodology is evaluated as a function of noise, overlap, relative intensity, and anisotropy difference between components using simulated mixtures of the DNA bases. The ability of this method to extract individual spectra from steady-state fluorescence data arrays is illustrated for mixtures containing two and three components.     

Intensity effects on the fluorescence of in vivo chlorophyll

A technique for measuring relative quantum yields of fluorescence with a picosecond streak camera is described. We show that Chlorella pyrenoidosa exhibit an intensity dependent quantum yield when irradiated with single picosecond light pulses. This effect also occurs under conditions that inhibit the activity of the reaction centres, which can therefore be excluded as the cause.When a pulse train (pulse separation 6.9 ns) was used, the quantum yield was further reduced by the light absorbed from previous pulses, which indicates the formation of a quenching species having a relatively long lifetime.Absolute quantum yields calculated from the fluorescence decay show that single excitation pulses of 3 · 10¹³ photons/cm² give results comparable to those obtained by very low intensity methods.