The polarization of fluorescence of DNA stains depends on the incorporation density of the dye molecules.

BACKGROUND: The fluorescence induced by polarized light sources, such as the lasers that are used in flow cytometry, is often polarized and anisotropic. In addition, most optical detector systems are sensitive to the direction of polarization. These two factors influence the accuracy of fluorescence intensity measurements. The intensity of two light sources can be compared only if all details of the direction and degree of polarization are known. In a previous study, we observed that fluorescence polarization might be modified by dye-dye interactions. This report further investigates the role of dye density in fluorescence polarization anisotropy. METHODS: We measured the polarization distribution of samples stained with commonly used DNA dyes. To determine the role of fluorophore proximity, we compared the monomeric and a dimeric form of the DNA dyes ethidium bromide (EB), thiazole orange (TO), and oxazole yellow (YO). RESULTS: In all dyes sampled, fluorescence polarization is less at high dye concentrations than at low concentrations. The monomeric dyes exhibit a higher degree of polarization than the dimeric dyes of the same species. CONCLUSIONS: The polarization of fluorescence from DNA dyes is related to the density of incorporation into the DNA helix. Energy transfer between molecules that are in close proximity loosens the linkage between the excitation and emission dipoles, thereby reducing the degree of polarization of the emission.     

Antibody-hapten interactions: circular and linear polarization of the fluorescence of dansyl bound to anti-dansyl antibodies

The fluorescence spectra of several dansyl derivatives (dansylamide, ?-N-dansyl-l-lysine, dansyl-l-alanine, and α-N-dansyl-l-alanine amide) bound to anti-dansyl antibodics (induced by an α-N-dansyl-poly d,l-alanine-poly l-lysine conjugate) are shifted by about 60 nm to the blue, and the quantum yields are markedly enhanced, compared to their respective fluorescence properties in water. The light emitted by the bound haptens is partly circularly polarized, reflecting the asymmetry induced in the bound chromophores by the antibody combining site. In contradistinction, the fluorescence spectrum of 1-dansyl-2-alanine diaminoethane bound to anti-alanine antibodies is similar to that of the free fluorophore in water and lacks circular polarization. These results imply that in this case the fluorophore of the hapten protrudes out of the site into the aqueous solvent. No circular dichroism is observed in the 300 to 400 nm region for the dansyl-anti-dansyl complex. Thus a change in the mode of interaction between the chromophore and its binding site takes place upon electronic excitation. The heterogeneity of the antibody binding sites is expressed by the dependence of the circular polarization of fluorescence on excitation wavelength. Differences in the circular polarization of luminescence were also observed when the residues attached to the dansyl group have been varied. This may reflect differences in the alignment of the fluorophore within the binding sites for the different dansyl derivatives.The linear polarization of dansylamide dissolved in glycerol is not constant across the emission band, indicating that the transition dipole moments related to the various vibronic states do not have the same spatial directions. Vibronic mixing of the emitting excited state with higher electronic states is thus indicated. Dansyl-l-alanine bound to anti-dansyl antibodies exhibitsan even more pronounced variation of the linear polarization across the emission band. In this case, the dependence of the linear polarization of the emitted light on excitation wavelength is anomalous, which is again a reflection of the heterogeneity of the population of the antibody molecules. The implications of these results to the studies of the fluorescence polarization of dansyl-protein complexes are discussed.     

Heterogeneity of binding sites of proflavin on DNA

The desorption and melting with temperature of proflavine–DNA complexes has been studied by spectrophotometry and spectrofluorometry. Two methods are described to determine at each temperature the concentration of free and bound dye. The first one is based on the quenching of fluorescence of the free dye by the iodine ion, the second on fluorescence polarization measurements. It is shown that the sites where the bound dye fluoresces are thermally less stable than those where it is quenched, in such a way that a redistribution of the dye between the two types of sites occurs at intermediate temperatures, leading to a drop in the total fluorescence. This confirms the nature of the “emitting” sites which correspond to AT-rich region, while “quenched” sites correspond to GC-rich region. The first have a larger binding constant at room temperature, but only the latter are stabilized by dye intercalation. The desorption and melting have also been followed through the relative changes of absorption. The curves obtained at different wavelengths are not superimposed which is at variance with what is observed with complexes of proflavine with poly dAT and poly dG.dC. The beginning of the desorption process corresponds to minor variations at 445 nm, the maximum of absorption of the free dye, but large changes occur at 460 nm, the maximum of the difference spectrum of the complexes proflavine–poly dAT and proflavine-poly dG.dC. The spreading of the melting curves for different wave lengths must therefore reflect the dependence of the absorption spectra of the dye on the nature of the neighboring bases. However, the action spectrum of the fluorescence, which gives the absorption spectrum of the “emitting” sites only, is identical with the total absorption spectrum of the bound dye.     

Spectroscopic investigations of the potential-sensitive membrane probe RH421.

The absorbance spectra, fluorescence emission and excitation spectra, and fluorescence anisotropy of the potential-sensitive styryl dye RH421 have been investigated in aqueous solution and bound to the lipid membrane. The potential-sensitive response of the dye has been studied using a preparation of membrane fragments containing a high density of Na+, K(+)-ATPase molecules. In aqueous solution the dye is sensitive both to changes in pH and ionic strength. Evidence has been found that the dye readily aggregates in aqueous solution. Aggregation is enhanced by an increase in ionic strength. The aggregates formed display a low fluorescence intensity. At high pH values (above approx. 8) changes in the dye's fluorescence spectra are observed, which may be due to a reaction of the dye with hydroxide ions. When bound to the membrane the dye also exhibits concentration-dependent fluorescence changes. The potential-sensitive response of the dye in Na(+),K(+)-ATPase membrane fragments after addition of MgATP in the presence of Na+ ions cannot be explained by a purely electrochromic mechanism. The results are consistent with either a potential-dependent equilibrium between membrane-bound dye monomers and membrane-bound dimers, similar to that previously proposed for the dye merocyanine 540, or with a field-induced structural change of the membrane.     

What causes the variation of polarization degree across the emission spectrum of proteins?

A gradual decrease in fluorescence polarization across the emission spectrum on increase in wavelength has been recorded for a number of proteins and also for tryptophan, N-acetyltryptophan and glycyltryptophan. Various factors responsible for this dependence have been analyzed. It is shown that if the emission originates from both the 1La and 1Lb states, the position and form of the fluorescence spectrum polarization components as well as the slope of the dependence of the degree of polarization upon emission wavelength must always vary with the excitation wavelength. However, this condition, although necessary, is not enough to prove the participation of 1Lb in emission. The dependence of the form of the emission polarization spectrum upon excitation wavelength obtained for some proteins is explained by tyrosine residues contributing to the emission. Consequently, there are no reasons for assuming that the 1Lb oscillator participates in emission. It has been observed that for individual emitting centres, the slope of the dependence of the degree of polarization upon emission wavelength is determined by alteration of the vibrational substates, between which the transition with radiation takes place. The heterogeneity in the microenvironment properties of separate tryptophan residues in multitryptophan proteins and the existence, under certain conditions, of a correlation between the radiative lifetime of the emitting centre (determining the degree of the emission polarization) and the completeness of the microenvironment orientational relaxation (determining the emitted quantum of energy) can also affect the slope of this dependence.     

Dynamics of carbohydrate residues of alpha 1-acid glycoprotein (orosomucoid) followed by red-edge excitation spectra and emission anisotropy studies of Calcofluor White

Dynamics studies on Calcofluor White bound to the carbohydrate residues of sialylated and asialylated alpha 1-acid glycoprotein (orosomucoid) have been performed. The interaction between the fluorophore and the protein was found to occur preferentially with the glycan residues with a dependence on their spatial conformation. In the presence of sialylated alpha 1-acid glycoprotein, excitation at the red edge of the absorption spectrum of calcofluor does not lead to a shift in the fluorescence emission maximum (440 nm) of the fluorophore. Thus, the emission of calcofluor occurs from a relaxed state. This is confirmed by anisotropy studies as a function of temperature (Perrin plot). In the presence of asialylated alpha 1-acid glycoprotein, red-edge excitation spectra show an important shift (8 nm) of the fluorescence emission maximum of the probe. This reveals that emission of calcofluor occurs before relaxation of the surrounding carbohydrate residues occurs. Emission from a non-relaxed state means that Calcofluor molecules are bound tightly to the carbohydrate residues, a result confirmed by anisotropy studies.     

Excitation energy transfer in the light-harvesting chlorophyll a/b.protein

The "light-harvesting chlorophyll a/b.protein" described by Thornber has been prepared electrophoretically from spinach chloroplasts. The optical properties relevant to energy transfer have been measured in the red region (i.e. 600-700 nm). Measurements of the absorption spectrum, fluorescence excitation spectrum and excitation dependence of the fluorescence emission spectrum of this protein confirm that energy transfer from chlorophyll b to chlorophyll a is highly efficient, as is the case in concentrated chlorophyll solutions and in vivo. The excitiation dependence of the fluorescence polarization shows a minimum polarization of 1.9% at 650 nm which is the absorption maximum of chlorophyll b in the protein and rises steadily to a maximum value of 13.8% at 695 nm, the red edge of the chlorophyll a absorption band. Analysis of these measurements shows that at least two unresolved components must be responsible for the chlorophyll a absorption maximum. Comparison of polarization measurements with those observed in vivo shows that most of the depolarization observed in vivo can take place within a single protein. Circular dichroism measurements show a double structure in the chlorophyll b absorption band which suggest an exciton splitting not resolved in absorption. Analysis of these data yields information about the relative orientation of the So leads to S1 transition moments of the chlorophyll molecules within the protein.     

Excited-state properties of chiral [4]helicene cations

The photophysical properties of a series of helicene cations in various solvents have been investigated using stationary and time-resolved spectroscopy. These compounds fluoresce in the near infrared region with a quantum yield ranging between 2 and 20% and a lifetime between 1 and 12 ns, depending of the solvent. No clear solvent dependence could be recognized except for a decrease of fluorescence quantum yield and lifetime with increasing hydrogen-bond donating ability of the solvent. In water, the helicene cations undergo aggregation. This effect manifests itself by the presence of a slow fluorescence decay component, whose amplitude increases with dye concentration, and by a much slower decay of the polarization anisotropy in water compared to an organic solvent of similar viscosity. However, aggregation has essentially no effect on the stationary fluorescence spectrum, whereas relatively small changes can be seen in the absorption spectrum. Analysis of the dependence of aggregation on the dye concentration reveals that the aggregates are mostly dimers and that the aggregation constant is substantially larger for hetero- than homochiral dimers.     

DNA torsional dynamics by multifrequency phase fluorometry.

The time decay of the fluorescence polarization anisotropy of calf thymus DNA-ethidium complexes is obtained from measurements with sine-modulated excitation employing the so-called multifrequency phase fluorometry. A torsional dynamics model developed by J. M. Schurr [(1984) Chemical Physics, Vol. 84, pp. 71-96] and translated into the frequency domain is found here to describe accurately DNA-ethidium fluorescence data collected under modulated excitation. At a low dye/DNA ratio (1:400) the value of the DNA torsional constant (alpha = 4.63 +/- 0.2 10(-12) dyne cm) fitting the data agrees very well with the known values of alpha. When the measurements are extended to a higher ethidium/DNA ratio, energy transfer effects between intercalated dyes are observed. A theoretical prediction of the donor and acceptor dye contributions to the fluorescence polarization anisotropy is made here, taking into account also dye-dye distance distributions.     

Excitation energy transfer in the light-harvesting chlorophyll

The “light-harvesting chlorophyll a/b · protein” described by Thornber has been prepared electrophoretically from spinach chloroplasts. The optical properties relevant to energy transfer have been measured in the red region (i.e. 600–700 nm). Measurements of the absorption spectrum, fluorescence excitation spectrum and excitation dependence of the fluorescence emission spectrum of this protein confirm that energy transfer from chlorophyll b to chlorophyll a is highly efficient, as is the case in concentrated chlorophyll solutions and in vivo. The excitation dependence of the fluorescence polarization shows a minimum polarization of 1.9 % at 650 nm which is the absorption maximum of chlorophyll b in the protein and rises steadily to a maximum value of 13.8 % at 695 nm, the red edge of the chlorophyll a absorption band. Analysis of these measurements shows that at least two unresolved components must be responsible for the chlorophyll a absorption maximum. Comparison of polarization measurements with those observed in vivo shows that most of the depolarization observed in vivo can take place within a single protein. Circular dichroism measurements show a doublet structure in the chlorophyll b absorption band which suggests an exciton splitting not resolved in absorption. Analysis of these data yields information about the relative orientation of the S₀→S₁ transition moments of the chlorophyll molecules within the protein.     

The interaction of quercetin with human serum albumin: a fluorescence spectroscopic study

Quercetin (3,3',4',5,7-pentahydroxyflavone), a ubiquitous, bioactive plant flavonoid, is known to possess anti-cancer, anti-tumor, and other important therapeutic activities of significant potency and low systemic toxicity. In this communication, we report for the first time a study on the interactions of quercetin with the plasma protein human serum albumin (HSA), exploiting the intrinsic fluorescence emission properties of quercetin as a probe. Quercetin is weakly fluorescent in aqueous buffer medium, with an emission maximum at approximately 538 nm. Binding of quercetin with HSA leads to dramatic enhancement in the fluorescence emission intensity and anisotropy (r), along with significant changes in the fluorescence excitation and emission profiles. The excitation spectrum suggests occurrence of efficient F?rster type resonance energy transfer (FRET) from the single tryptophan-214 residue of HSA to the protein bound quercetin. The emission, excitation, and anisotropy (r=0.18 at [HSA]=30 microM) data (using the native protein) along with emission studies of quercetin using partially denatured HSA (by 8M urea) indicate that the quercetin molecules bind at a motionally restricted site near tryptophan-214 in the interdomain cleft region of HSA. Furthermore, the binding constant (K=1.9 x 10(5)M(-1)) and Gibbs free energy change (deltaG(0)=-30.12 kJ/mol)) for quercetin-HSA interaction have been calculated from the relevant anisotropy data. Implications of these results are examined, particularly in relation to prospective applications in biomedical research.     

Myoplasmic binding of fura-2 investigated by steady-state fluorescence and absorbance measurements.

Binding of the fluorescent Ca2+ indicator dye fura-2 by intracellular constituents has been investigated by steady-state optical measurements. Fura-2's (a) fluorescence intensity, (b) fluorescence emission anisotropy, (c) fluorescence emission spectrum, and (d) absorbance spectra were measured in glass capillary tubes containing solutions of purified myoplasmic proteins; properties b and c were also measured in frog skeletal muscle fibers microinjected with fura-2. The results indicate that more than half, and possibly as much as 85%, of fura-2 molecules in myoplasm are in a protein-bound form, and that the binding changes many properties of the dye. For example, in vitro characterization of the Ca2+-dye reaction indicates that when fura-2 is bound to aldolase (a large and abundant myoplasmic protein), the dissociation constant of the dye for Ca2+ is three- to fourfold larger than that measured in the absence of protein. The problems raised by intracellular binding of fura-2 to cytoplasmic proteins may well apply to cells other than skeletal muscle fibers.     

A fluorescence photobleaching study of the microsecond reorientational motions of DNA.

We have conducted a polarized fluorescence photobleaching recovery (FPR) study of the rotational dynamics of ethidium azide labeled DNA. Polarized photobleaching experiments provide data on microsecond and millisecond molecular reorientation that complement the information available from nanosecond fluorescence depolarization studies. In polarized FPR experiments an anisotropic angular concentration of fluorophore is created by bleaching dye molecules in a preferred orientation with a short, intense pulse of polarized light. The sample is then weakly illuminated, and the temporal variation in the emitted fluorescence is monitored. The fluorescence signal will systematically change as molecules undergo post-bleach reorientation and the angular distribution of dye tends toward isotropy. We have observed that the time dependence of our microsecond FPR curves is also determined in part by nonrotational phenomena. To isolate the reorientational recovery we conduct our FPR experiments in two modes (called parallel and perpendicular) that differ only in the polarization of the bleaching light. A quotient function, R(t), is constructed from the data obtained in these two modes; the variation with time of this new quantity is governed solely by processes that are sensitive to the polarization of the incident light (e.g., molecular rotation). It is found experimentally that R(t) remains constant, as expected, for rotationally restricted DNA systems despite a temporal recovery in the parallel and perpendicular FPR curves. We also follow the dynamics of solutions of phage lambda DNA as revealed in the temporal dependence of R(t). This DNA system rotationally relaxes after approximately 100 microseconds and the dye/DNA complex reorients substantially during the 10-microseconds bleach period. Our FPR data are interpreted in terms of dynamic models of DNA motion.     

Coenzyme interaction with horse liver alcohol dehydrogenase. Evidence for allosteric coenzyme binding sites from thermodynamic equilibrium studies.

The techniques of fluorescence enhancement, fluorescence quenching, fluorescence polarization, and equilibrium dialysis are utilized to study the binding properties of coenzyme to horse liver alcohol dehydrogenase. Polarization of fluorescence and equilibrium dialysis show that NADH binds to alcohol dehydrogenase with a stoichiometry of 6 mol per mol of enzyme, in contrast to the value of 2 determined from fluorescence enhancement measurements. NAD+ also binds with a stoichiometry of six as was determined by equilibrium dialysis. The two NADH sites which bind coenzyme more tightly and which are revealed by fluorescence enhancement measurements are designated the catalytic sites. Binding of coenzyme to the four ancillary sites does not alter the quantum yield of NADH but results in a 20% contribution to quenching of enzyme's tryptophan fluorescence. From the emission anisotropy of bound NADH of 24.0% for the additional sites and 28.1% for the catalytic sites and their relative fluorescence lifetimes at the same wavelengths of excitation and emmision, we conclude that the nicotinamide ring of NADH bound to the additional sites exhibits a freedom of motion independent of the macromolecule, while that bound to the catalytic sites is more rigidly held. Polarization of fluorescence yields negative intrinsic free energies of 9.2 and 7.5 Cal M-1 for NADH interaction with the catalytic and additional sites, respectively. Although these values are 1.3 to 2.0 Cal higher than those determined by fluorescence quenching and equilibrium dialysis, the mean Hill coefficient of 1.76 plus or minus 0.06, the titration span of 2.4 logarithmic units and coupling free energies (in magnitude and sign) are the same for all these techniques. The above difference in the intrinsic free energies are attributed largely to the different modes of interaction of excited and unexcited NADH molecules with alcohol dehydrogenase.     

The interaction between heparin and antithrombin III: a comparison of two different heparin-dye conjugates

The interactions of antithrombin III with two heparin-dye conjugates have been compared using their fluorescence anisotropy. The first, heparin labelled with 5-isothiocyanatofluorescein, where the dye was mostly bound to unsulphated glucosamine residues, exhibited binding which was characteristic of heparin with a low affinity for antithrombin III. The second, heparin labelled with a reactive naphthalene dye (DENMT), showed similar binding character. However, when the heparin was treated with an amino group blocking agent prior to labelling with DENMT, the resultant heparin-dye conjugate showed binding behaviour, the strength of which was consistent with heparin molecules having both high and low affinity for antithrombin III. Heparin molecules with a high affinity for antithrombin III did not possess free amino groups. The implications of these findings are discussed with regard to the reliability of the data obtained using heparin-fluorescein conjugates.     

Proximity of lectin receptors on the cell surface measured by fluorescence energy transfer in a flow system.

Molecules of the lectin concanavalin A have been labeled separately with the fluorescein and rhodamine chromophores and jointly bound to the surface of transformed Friend erythroleukemia cells. The two dyes constitute an ideal donor-acceptor pair for fluorescence resonance energy transfer thereby permitting the determination of the proximity relationships between bound ligand molecules and the corresponding surface receptors. The transfer efficiency at saturation (about 57%) was measured in a multiparameter flow system using laser excitation at 488 nm and detection of fluorescein and rhodamine emission intensities as well as the emission anisotropy of the rhodamine fluorescence for each cell. The degree of energy transfer was estimated from the quenching of donor emission, the sensitization of acceptor emission, and the depolarization of acceptor fluorescence. The system has been modeled according to a formalism developed by Gennis and Cantor (Biochemistry 11: 2509, 1972). We estimate the separation between the surfaces of bound lectin molecules at saturation to be 0-40 A, a range possibly characteristic for micropatches induced by ligand binding.     

Orientation and spectral properties of two stilbazolium merocyanine dyes in stretched and unstretched polyvinyl alcohol films

Spectral properties (anisotropy coefficients calculated for absorption, emission and fluorescence decay time) of two stilbazolium merocyanine dyes have been determined to evaluate the applicability of these dyes as sensitizers in photodynamic therapy. The dyes were embedded in an anisotropic polymer matrix. Analysis of the emission decay components measured in polarized light provides information on the interactions of the dye molecules with the polymer matrix being a model of an anisotropic biological system. Different values of the emission anisotropies obtained from various polarized components of fluorescence decays have shown that the orientations of the dye molecules influence their interactions with the polymer. This means that differently oriented dye molecules located in biological systems should exhibit different interactions with membranes. The chain length and type of side groups attached as well as the salt form of the dye molecule were shown to influence the dye-polymer interactions and should be taken into account before the application of merocyanine dyes in medicine. These dyes seem to be promising optical sensors with spectral properties, including the calculated anisotropy coefficients, sensitive to the molecular environment, useful to study orientation and interaction with neighbouring molecules in biological membranes.     

Fluorescence imaging of two-photon linear dichroism: cholesterol depletion disrupts molecular orientation in cell membranes

The plasma membrane of cells is an ordered environment, giving rise to anisotropic orientation and restricted motion of molecules and proteins residing in the membrane. At the same time as being an organized matrix of defined structure, the cell membrane is heterogeneous and dynamic. Here we present a method where we use fluorescence imaging of linear dichroism to measure the orientation of molecules relative to the cell membrane. By detecting linear dichroism as well as fluorescence anisotropy, the orientation parameters are separated from dynamic properties such as rotational diffusion and homo energy transfer (energy migration). The sensitivity of the technique is enhanced by using two-photon excitation for higher photo-selection compared to single photon excitation. We show here that we can accurately image lipid organization in whole cell membranes and in delicate structures such as membrane nanotubes connecting two cells. The speed of our wide-field imaging system makes it possible to image changes in orientation and anisotropy occurring on a subsecond timescale. This is demonstrated by time-lapse studies showing that cholesterol depletion rapidly disrupts the orientation of a fluorophore located within the hydrophobic region of the cell membrane but not of a surface bound probe. This is consistent with cholesterol having an important role in stabilizing and ordering the lipid tails within the plasma membrane.     

A theory for polarized fluorescence microscopy of chromosome structures

A theory for the determination of DNA arrangements in DNA-containing specimens, using planar aromatic dye molecules as probes for plane polarization of fluorescence, has been described. At low dye-to-DNA concentrations, the dye molecules are sandwiched between the stacked bases of DNA; hence, the fluorescence from the dye bound to a local region of DNA helix is plane-polarized with the polarization direction perpendicular to the local axis of DNA. The degree of such polarization from an aligned DNA-specimen complexed with dye is determined both by the DNA orientation and the conformational state (e.g., base tilt) of DNA into that specimen. Analysis has been made of the relationship between the degree of polarization and the orientation of the emitting dipoles of dye. The dye complexes may be aligned in a mechanical shear or electric field. However, any change in the orientation distribution of the emitting dipoles due to force fields should be taken into account. With some assumptions and approximations, the magnitude and the direction of maximum polarization can be related to different orders of DNA coiling and to their various combinations. Since the measured polarization is averaged over all DNA regions of the specimen, if the magnitude of polarization is appreciable and the polarization occurs in the specific direction of the specimen, the theory helps to eliminate several probable arrangements of DNA. The predominant molecular features of the actual DNA arrangement can be determined through this process of elimination, as explained in two subsequent papers with T-even bacteriophage and chromosome systems.     

Cytochrome c interaction with membranes. Absorption and emission spectra and binding characteristics of iron-free cytochrome c.

A cytochrome c derivative from which iron is removed has been prepared and characterized. Several lines of evidence indicate that native and porphyrin cytochrome c have similar conformations: they have similar elution characteristics on Sephadex gel chromatography; in both proteins the tryptophan fluorescence is quenched and the pK values of protonation of the porphyrin are identical. Porphyrin cytochrome c does not substitute for native cytochrome c in either the oxidase reaction or in restoring electron transport in cytochrome-c-depleted mitochondria. It does however competitively inhibit native cytochrome c in these reactions, the Ki for inhibition being larger than the Km for reaction. The absorption and emission spectra, and the polarized excitation spectrum of the porphyrin cytochrome c are characteristic of free base porphyrin. The absence of fluorescence quenching of porphyrin cytochrome c when the protein is bound to cytochrome oxidase suggests that heme to heme distance between these proteins is larger than 0.5 to 0.9 nm depending upon orientation. Binding of the porphyrin cytochrome c to phospholipids or to mitochondria increases the fluorescence polarization of a positively polarized absorption band, which indicates that the bound form of the protein does not rotate freely within the time scale of relaxation from the excited state.