Biophysical analysis of phaseolin denaturation induced by urea,guanidinium chloride,pH, and temperature

The structural stability of phaseolin was determined by using absorbance, circular dichroism (CD), fluorescence emission, and fluorescence polarization anisotropy to monitor denaturation induced by urea, guanidinium chloride (GdmCl),pH changes, increasing temperature, or a combination thereof. Initial results indicated that phaseolin remained folded to a similar extent in the presence or absence of 6.0 M urea or GdmCl at room temperature. In 6.0 M GdmCl, phaseolin denatures at approximately 65°C when probed with absorbance, CD, and fluorescence polarization anisotropy. The transition occurs at lower temperatures by decreasingpH. Kinetic measurements of denaturation using CD indicated that the denaturation is slow below 55°C and is associated with an activation energy of 52 kcal/mol in 6.0 M GdmCl. In addition, kinetic measurement using fluorescence emission indicated that the single tryptophan residue was sensitive to at least two steps of the denaturation process. The fluorescence emission appeared to reflect some other structural perturbation than protein denaturation, as fluorescence inflection occurred approximately 5°C prior to the changes observed in absorbance, CD, and fluorescence polarization anisotropy.     

Enhancement of Emission Efficiency of Deep-Ultraviolet AlGaN Quantum Wells Through Surface Plasmon Coupling with an Al Nanograting Structure

The enhancement of the internal quantum efficiency (IQE) of deep-ultraviolet Al _x Ga_1-x N/Al _y Ga_1-y N (x < y) quantum wells (QWs) by fabricating one-dimensional Al nanogratings on a QW structure for inducing surface plasmon (SP) coupling is demonstrated. Through temperature-dependent photoluminescence (PL) measurement, the enhancements of IQE in different emission polarizations are illustrated. Due to the small difference in energy band level between the heavy/light hole and split-off valence bands, the IQEs of the transverse electric- (TE-) and transverse magnetic- (TM-) polarized emissions are about the same. When emission polarization is perpendicular to Al-grating ridges, the SP resonance mode for coupling with the QWs is dominated by localized surface plasmon (LSP). When emission polarization is parallel with Al-grating ridges, the coupled SP resonance mode may mix LSP and SP polariton. In this polarization, LSP can be excited because of the width fluctuation of a grating ridge. When the excitation laser polarization is perpendicular to Al-grating ridges, the strong LSP resonance at the excitation laser wavelength leads to stronger excitation and hence higher IQE levels.     

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.     

Two effects of electrical fields on chloroplasts

An electrical field across a suspension of Chenopodium chloroplasts stimulates the emission of delayed light during the time the field is on. This stimulation can be used to calculate the distance over which the electron moves in the untrapping process that gives the delayed light. An electrical field applied at the time of illumination gives a polarization to the suspension of chloroplasts that lasts for some seconds. This polarization is a new way to study delayed light and fluorescence from chloroplasts.     

Anisotropy of the emission and absorption bands of spinach chloroplasts measured by fluorescence polarization and polarized excitation spectra at low temperature

Spectra of fluorescence polarization were measured between 4 and 120 K of spinach chloroplasts, oriented in a magnetic field. At least seven emission bands were observed. The well known bands near 685 nm (‘F-685’) and 735–740 nm (‘F-735’) and the band near 680 nm (‘F-680’) were strongly polarized parallel to the plane of the thylakoid membrane, whereas emission bands near 695 nm (‘F-695’), 710, 730–735 and 760 nm showed perpendicular polarization. Assuming perfect orientation of the thylakoid membranes, we calculated orientation angles of 64, 47 and 66.5° for the emission dipoles of F-685, F-695 and F-735, respectively, with respect to the normal of the membrane. Excitation spectra of F-695 and F-735 in polarized light at 4 K provided information about the orientation of the absorption dipoles of chlorophylls a and b. The spectra thus obtained were in very good agreement with the linear dichroism spectrum. Moreover, they allowed us to distinguish between the pigments associated with Photosystems I and Ii, which is not possible from measurement of linear dichroism alone. The results indicate that a high degree of orientation is not confined to the long-wave absorbing bands, but also bands at shorter wavelength show a clear anisotropy. The calculated orientations were in quantitative agreement with the hypothesis that F-685 and F-735 are associated with chlorophylls absorbing at 676 and 710–715 nm, respectively.     

Luminescence of bacteriorhodopsin from Halobacterium halobium and its connection with the photochemical conversions of the chromophore

Red luminescence of purple membranes from Halobacterium halobium cells in suspension, dry film or freeze-dried preparations was studied and its emission, excitation and polarization spectra are reported. The emission spectra have three bands at 665–670, 720–730 and at 780–790 nm. The position (maximum at 580 nm) and shape of the excitation spectra are close to those of the absorption spectra. The spectra depend on experimental conditions, in particular on pH of the medium. Acidification increases the long wavelength part of the emission spectra and shifts the main excitation maximum 50–60 nm to the longer wavelength side. Low-temperature light-induced changes of the absorption, emission and excitation spectra are presented. Several absorbing and emitting species of bacteriorhodopsin are responsible for the observed spectral changes. The bacteriorhodopsin photoconversion rate constant was estimated to be about 1 · 10¹¹ s^?1 at ? 196°C from the quantum yields of the luminescence (1 · 10^?3) and photoreaction (1 · 10^?1). The temperature dependence of the luminescence quantum yield points to the existence of two or three quenching processes with different activation energies. High degree of luminescence polarization (about 45–47%) throughout the absorption and fluorescence spectra and its temperature independence show that there is no energy transfer between bacteriorhodopsin molecules and no chromophore rotation during the excitation lifetime. In carotenoid-containing membranes, energy migration from the bulk of carotenoids to bacteriorhodopsin was not found either. Bacteriorhodopsin phosphorescence was not observed in the 500–1100 nm region and the emission is believed to be fluorescence by nature.     

DNA ORGANIZATION IN THE MATURE SPERM OF SEVERAL ORTHOPTERA BY THE METHOD OF POLARIZED FLUORESCENCE MICROSCOPY

Mature sperm of Acheta domesticus, Acheta assimilis, Nemobius fasciatus, Nemobius confusus, Melanoplus femur-rubrum, Romalea microptera, Scudderia curvicauda, and Ceuthophilus nigricans were examined for DNA configuration by means of polarized fluorescence microscopy. In all cases, the results suggest that the DNA lies in unsupercoiled array, predominantly parallel to the elongate sperm head axes. Detailed calculations of the factors influencing the degree of polarization of the fluorescent emission from supercoiled DNA are contained in an appendix.     

Strong Near-infrared Avalanche Photoluminescence from Ag Nanowire Arrays

Ag nanowire (NW) arrays with NW diameter d _NW?=?12–120 nm were electrodeposited in anodic aluminum oxide templates. Strong avalanche photoluminescence (PL) from Ag NW arrays with small d _NW were observed near 914 nm by using picosecond laser at the excitation wavelength 808 nm, which is originated from the plasmon-enhanced radiative intraband transitions. The peak PL intensity of the avalanche PL from the sample with small diameter d _NW?=?12 nm is about 10² times stronger than that of the linear PL from the sample with large diameter d _NW?=?120 nm. The opposite excitation polarization dependence and emission polarization distribution of the PL from Ag NW array with d _NW?=?12 nm and d _NW?=?120 nm were also observed.     

Fluorescence properties of the light-harvesting bacteriochlorophyll protein from Rhodopseudomonas sphaeroides R-26

The light-harvesting bacteriochlorophyll-protein (BChl-protein) from Rhodopseudomonas sphaeroides, R-26 mutant, exhibits a strong optical absorption peak near 850 nm (Q_y band) and a weaker peak at 590 nm (Q_x band). This pigment-protein appears to contain two BChl molecules per subunit, and previous circular dichroism studies indicated the presence of excitonic interactions between the BChl molecules. The complex exhibits a fluorescence maximum near 870 nm at room temperature. Excitation in the Q_y region results in polarization p values that vary only from +0.12 at 820 nm to +0.14 near 900 nm. These values are appreciably smaller than that for monomeric BChl in viscous solvents (p > 0.4). By contrast, using Q_x excitation the p value is ?0.25 for the BChl-protein complex, which is close to that observed for the BChl monomer. For the BChl-protein these polarization values do not change greatly at a temperature of 90 K; however, the Stokes' shift of the fluorescence emission increases significantly over that at room temperature.     

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.     

The fluorescein-mediated interaction of bovine serum albumin with fluorescent derivatives of prolactin and other polypeptides in polarization of fluorescence based assays

During the course of studies relating to the interaction of bovine prolactin with its receptor, it was observed that the fluorescence polarization of prolactin labeled with fluorescein isothiocyanate (fluorescein prolactin) increased from 0.10 to 0.15 upon the addition of bovine serum albumin. Dilution titration measurements show an apparent K_dissociation for the BSA-fluorescein-prolactin complex of 1.1 × 10^?7 M. The stoichiometry of the complex was shown to be approximately 2 mol of fluorescein-prolactin per mole of BSA. The fluorescence emission spectra of the fluorescein moiety in the fluorescein-prolactin is slightly red shifted and increased in intensity in the presence of BSA. The interaction between prolactin and BSA is dependent on the fluorescein attached to the prolactin since [¹²⁵I]prolactin does not form a complex with BSA under identical conditions. The fluorescence polarization of fluorescein-labeled growth hormone and α-lactalbumin also increased in the presence of BSA, suggesting that BSA may interact generally with fluorescein-labeled proteins to form complexes bridged through the fluorescein moiety.     

Involvement of mitochondria in changes in fluorescein excitation and emission polarization spectra in living cells.

The comparison of fluorescein polarization spectra in living cells and in isolated subcellular structures identified the mitochondria as the cytoplasmic domain in which on excitation at 470 nm the sharp fluorescein emission polarization peak at 510 nm is formed. Changes in the emission polarization peak during the cell cycle or those induced by growth stimulators and inhibitors reflect structural changes in the mitochondria on their transition from the resting, orthodox into the active, ATP-generating, condensed conformation and vice versa. Possible mechanisms for the formation of the sharp emission polarization peak are discussed.     

Pigment organization of the B800–850 antenna complex of Rhodopseudomonas sphaeroides

The B800–850 antenna complex of Rhodopseudomonas sphaeroides was studied by comparing the spectral properties of several different types of complexes, isolated from chromatophores by means of the detergents lithium dodecyl sulfate (LDS) or lauryl dimethylamine N-oxide (LDAO). Fluorescence polarization spectra of the BChl 800 emission at 4 K indicated that rapid energy transfer between at least two BChl 800 molecules occurs with a rate constant of energy transfer k_ET > 3 · 10¹² s^?1. The maximal dipole-dipole distance between the two BChl 800 molecules was calculated to be 18–19 Å. The porphyrin rings of the BChl 800 molecules are oriented parallel to each other, while their Q_y transition moments are mutually perpendicular. The energy-transfer efficiency from carotenoid to bacteriochlorophyll measured in different complexes showed that two functionally different carotenoids are present associated with, respectively, BChl 800 and BChl 850. Fluorescence polarization and linear dichroism spectra revealed that these carotenoids have different absorption spectra and a different orientation with respect to the membrane. The carotenoid associated with BChl 800 absorbs some nanometers more to the red and its orientation is approximately parallel to the membrane, while the carotenoid associated with BChl 850 is oriented more or less perpendicular to the membrane. The fluorescence polarization of BChl 850 was the same for the different complexes. This indicates that the observed polarization of the fluorescence is determined by the smallest complex obtained which contains 8–10 BChl 850 molecules. The B800–850 complex isolated with LDAO thus must consist of a highly ordered array of smaller structures. On basis of these results a minimal model is proposed for the basic unit consisting of four BChl 850 and two BChl 800 and three carotenoid molecules.     

Spatial and temporal electroselection patterns in electric field stimulation of polarized luminescence from photosynthetic membrane vesicles

Electroselection processes of charge recombination are manifested in the study of electric field induced polarized emission from photosynthetic membrane vesicles. The study explores the coupled spatial-temporal characteristics of electric field induced charge recombination by examining the dependence of the integrated polarized emission and the time dependent polarization on electric field strength. The experimental results were fitted to theoretical models by computer simulations employing empirical parameters. Simulation of the dependence of the integrated polarized components of emission on electric field strength, suggests field-dependent increased ratio between radiative and nonradiative rates of charge recombination. The observation that the initial polarization values are independent of electric field strength supports the assumption that electric field induced emission originates from the pole area and then spreads away from it towards the equator. The propagation rate of this electric field induced charge recombination from the pole area towards the equator is reflected by the decay of polarization which increases upon raising the electric field strength. Simulation of the polarization's decay, based on a calculated angle of 26.3 ± 0.4° between the transition moment of emission and the plane of the membrane, establishes coupled temporal spatial patterns of electroselection in intramembrane electron transfer invoked by exposing preilluminated photosynthetic vesicles to a homogeneous electric field.     

Influence of membrane lipids on the photochemistry of bacteriorhodopsin in the purple membrane of Halobacterium halobium

Purple membrane fragments from Halobacterium halobium were reconstituted with the native lipids replaced by dipalmitoyl phosphatidylcholine and by egg lecithin. In parallel studies the temperature dependence of bacteriorhodopsin phototransient lifetime and absorption dichroism and of in situ lipid microviscosity were determined; the former two by, respectively, conventional and polarization flash photometry, and the latter by observation of emission depolarization of an embedded fluorescent dye, 1,6-diphenyl-1,3,5-hexatriene. Discontinuities in lipid microviscosity profiles in native and egg lecithin purple membrane were reflected in both the photochemical cycle frequency and bacteriorhodopsin chromophore rotational mobility. The influence exerted by membrane-lipid viscosity appears to be a secondary effect, and points to the bacteriorhodopsin chromophoric group being situated in the protein interior.     

Fluorescence Polarization Studies of the Binding of BMS 181176 to DNA

Abstract

The DNA binding of BMS 181176, an antitumor antibiotic derivative of rebeccamycin was characterized by DNA unwinding assays, as well as by fluorescence emission and polarization spectroscopic techniques. Unwinding and rewinding of supercoiled DNA was interpreted in terms of intercalation of BMS 181176 into DNA BMS 181176 shows an enhanced fluorescence emission upon binding to the AT sequence and no enhancement upon binding to the GC sequence. BMS 181176 appears to be a weaker binder to poly(dAdT).poly(dAdT) compared to doxorubicin and ethidium bromide. When bound to DNA, the rotational motion of BMS 181176 is substantially decreased as evident from the increase in fluorescence polarization. BMS 181176 exhibits a range of binding strengths depending on the DNA This is demonstrated by the Acridine Orange displacement assay using fluorescence polarization.     

Fluorescence polarization spectroscopy and time-resolved fluorescence kinetics of native cancerous and normal rat kidney tissues.

Steady state fluorescence polarization spectra and time-resolved emission decay kinetics have been measured in vitro from malignant and normal rat kidney tissue. The degrees of polarization and emission lifetimes from the cancerous and normal systems are different. The spectroscopic differences are attributed to environmental transformations local to the native flavin and porphyrin fluorophors' binding sites.     

Biophysical analysis of phaseolin denaturation induced by urea, guanidinium chloride, pH, and temperature.

The structural stability of phaseolin was determined by using absorbance, circular dichroism (CD), fluorescence emission, and fluorescence polarization anisotropy to monitor denaturation induced by urea, guanidinium chloride (GdmCl),pH changes, increasing temperature, or a combination thereof. Initial results indicated that phaseolin remained folded to a similar extent in the presence or absence of 6.0 M urea or GdmCl at room temperature. In 6.0 M GdmCl, phaseolin denatures at approximately 65°C when probed with absorbance, CD, and fluorescence polarization anisotropy. The transition occurs at lower temperatures by decreasingpH. Kinetic measurements of denaturation using CD indicated that the denaturation is slow below 55°C and is associated with an activation energy of 52 kcal/mol in 6.0 M GdmCl. In addition, kinetic measurement using fluorescence emission indicated that the single tryptophan residue was sensitive to at least two steps of the denaturation process. The fluorescence emission appeared to reflect some other structural perturbation than protein denaturation, as fluorescence inflection occurred approximately 5°C prior to the changes observed in absorbance, CD, and fluorescence polarization anisotropy.     

The constituent tryptophans and bisANS as fluorescent probes of the active site and of a secondary binding site of stromelysin-1 (MMP-3)

The active site of the catalytic domain of stromelysin-1 (matrix metalloproteinase-3, MMP-3) was probed by fluorescence quenching, lifetime, and polarization of its three intrinsic tryptophans and by the environmentally sensitive fluorescent reporter molecule bisANS. Wavelength-dependent acrylamide quenching identified three distinct emitting tryptophan species, only one of which changes its emission and fluorescence lifetime upon binding of the competitive inhibitor Batimastat. Significant changes in the tryptophan fluorescence polarization occur upon binding by any of the three hydroxamate inhibitors Batimastat, CAS108383-58-0, and Celltech CT1418, all of which bind in the P2′-P3′ region of the active site. In contrast, the inhibitor CGS27023A, which is t hought to bind in the P1-P1′ region, does not induce any change in tryptophan fluorescence polarization. The use of the fluorescent probe bisANS revealed the existence of an auxiliary binding site extrinsic to the catalytic cleft. BisANS acts as a competitive inhibitor of stromelysin with a dissociation constant ofK _i=22 μM. In addition to this binding to the active site, it also binds to the auxiliary site with a dissociation constant of 3.40±0.17 μM. The auxiliary site is open, hydrophobic, and near the fluorescing tryptophans. The binding of bisANS to the auxiliary site is greatly enhanced by Batimastat, but not by the other competitive inhibitors tested.