Fluorescence properties of free and protein bound fluorescein dyes. I. Macrospectrofluorometric measurements.

Excitation and emission properties of fluorescein derivatives were studied macrofluorometrically. Measurements were performed with solutions of various concentrations (0.07-100 microgram/ml) of free sodium fluorescein prepared from fluorescein diacetate (FDA), fluorescein isothiocyanate (FITC) and FITC bound to rabbit gamma-globulin. Both excitation and emission spectra as well as fluorescence intensities at constant excitation/emission wavelengths (496/515 nm) were recorded. The findings indicate that (1) FDA gives about twice the fluorescence intensity compared to equal concentrations of FITC. (2) The fluorescence properties of FITC upon excitation with blue light (lambda = 496 nm) are only slightly altered by the conjugation to rabbit gamma-globulin. (3) Considerable quenching due to conjugation could, however, be shown to occur upon UV excitation (lambda = 340 nm). (4) Fluorescence emission excited by visible blue light (496 nm) increases linearly to dye concentration in a range of 0.07-2.5 microgram/ml. Beginning at 5 microgram/ml (10-(5) M/1) all three compounds show a sharp decrease of fluorescence intensity with further increasing concentration. Practical aspects of these data for the immunofluorescence method are discussed.     

Fluorescein excitation and emission polarization spectra in living cells: changes during the cell cycle.

Changes in the fluorescein fluorescence emission and excitation polarization spectra in synchronized cultured S3 fibroblasts at G1, mid-S, and mitosis, as well as in human lymphocytes before and after stimulation with mitogens, were studied. In contrast to those measured in aqueous solutions the emission and excitation polarization spectra in living cells exhibit a wavelength dependence characteristic for the state of the cell cycle. Changes in the temperature and in the amount of intracellular water result in quantitative wavelength-independent changes in the polarization spectra. Possible mechanisms for the qualitative wavelength-dependent changes in the fluorescein emission and excitation polarization spectra during the cell cycle are discussed.     

Vector Alkaline Phosphatase Substrate Blue III: One Substrate for Brightfield Histochemistry and High-resolution Fluorescence Imaging by Confocal Laser Scanning Microscopy

A number of histochemical chromogenic substrates for alkaline phosphatase are commercially available and give reaction products with a range of colours for brightfield examination. Some of these reaction products are also fluorescent, exhibiting a wide excitation range and a broad emission peak. We report here that one of these substrates, Vector Blue III, yields a stable, strongly fluorescent reaction product with an excitation peak around 500 nm and a large Stokes shift to an emission peak at 680 nm. The reaction product can be excited using a mercury lamp with a fluorescein excitation filter or an argon ion laser at 488 nm or 568 nm, and the emission detected using a long-pass filter designed for Cy-5. Thus, a single substrate is suitable for brightfield imaging of tissue sections and high-resolution analysis of subcellular detail, using a confocal laser scanning microscope, in the same specimen.     

Fluorescein conjugates of 9- and 10-hydroxystearic acids: synthetic strategies, photophysical characterization, and confocal microscopy applications

Different strategies are presented to conjugate a fluorescein moiety to 9- and 10-hydroxystearic acids (HSAs). 5-Amino-fluorescein (5-AF) was used as a starting reagent. When reacted with acyl-chloride-modified HSAs, 5-AF gave rise to stable amide derivatives with a 75% reaction yield. These products exhibited the typical steady-state and time-resolved fluorescence properties of the fluorescein chromophore with absorption at 494 nm and emission at 519 nm. Flow cytometry studies confirmed the distinct proapoptotic effect of underivatized 9-HSA on Jurkat cells and revealed a comparable ability of its amide derivative. Confocal microscopy imaging studies showed that green fluorescence could stain intracellular membranous structures. Moreover, dual-dye labeling with Mito Tracker Red, followed by colocalization analysis, revealed that HSA can move to the mitochondria. Thus, fluorescent derivatives of HSA can be used to monitor the localization of these biologically active molecules in living cells and can provide a useful tool for linking biochemical investigation with optical visualization methods. In contrast, when unmodified HSAs were used, the reaction gave monoesterified and diesterified fluorescein derivatives. These products exhibited unusual steady-state and time-resolved fluorescence properties with the excitation wavelength at 342 nm and the emission wavelength at 432 nm. It is shown that the synthesized HSA amides of fluorescein provide all of the typical photophysical and instrumental advantages of this popular dye, whereas the unusual luminescence and excitation properties of the monoester and diester of the 5-aminofluorescein would make these dyes interesting to explore as potential candidates for two photon excitation applications.     

Discrete bathochromic shifts exhibited by fluorescein ligand bound to rabbit polyclonal anti-fluorescein Fab fragments

Eleven individual hyperimmune rabbit polyclonal anti-fluorescein Fab fragment preparations were resolved into heterogeneous subfractions based on differential dissociation times from a specific adsorbent. Four Fab subfractions (i.e., 0.1-, 1.0-, 10-, and 100-day elutions) that differed in affinity were characterized and classified according to the extent of the bathochromic shift in the absorption properties of antibody-bound fluorescein ligand. Absorption maxima of bound fluorescein were shifted in all cases to two distinct narrow ranges, namely, 505 to 507 nm or 518 to 520 nm relative to 491 nm for free fluorescein. There was no direct correlation between the two spectral shift populations and antibody affinity, fluorescence polarization, fluorescence quenching, or fluorescence lifetimes of bound ligand. Fluorescence emission maxima varied with the bathochromic shift range. Bound fluorescein ligand, with absorption maxima of 505 to 507 nm and 518 to 520 nm showed fluorescence emission maxima of 519 to 520 nm and 535 nm, respectively. The two spectral shift ranges differed by 14 to 15 nm and/or energies of 1.5 kcal mol^–1 relative to each other and to the absorption maximum for free fluorescein. Spectral effects on the antibody-bound ligand were discussed relative to solvent-water studies and the atomic structure of a high-affinity liganded anti-fluorescein active site.     

Fluorescence of equine platelet tropomyosin labeled with acrylodan

Equine platelet tropomyosin was labeled with the sulfhydryl-specific fluorescent reagent 6-acryloyl-2-dimethylaminonaphthalene (acrylodan). The extent of labeling at 4 degrees C could be regulated between 0.5 and 1.3 acrylodans per tropomyosin chain by varying the reaction time from 1 to 4.5 h. Acrylodan-labeled platelet tropomyosin, AD-P-TM, was highly fluorescent, having an emission maximum near 518 nm on excitation at 365 nm. Steady-state measurements of polarization of the fluorescence of AD-P-TM in both low and high ionic strength solutions gave Perrin plots that exhibited sharp changes in slope near 50 degrees C, indicative of a sharp increase in mobility of the label at that temperature. This correlates with the melting temperature of the platelet tropomyosin coiled coil observed by circular dichroism [G. P. C?té, W. G. Lewis, M. D. Pato, and L. B. Smillie, (1978) FEBS Lett. 91, 237-241]. Perrin plots of carboxypeptidase A-treated platelet tropomyosin that was labeled with acrylodan after digestion resembled more closely those of acrylodan-labeled cardiac tropomyosin rather than those of AD-P-TM, suggesting that the observed emission arose from label at Cys-153 on each truncated platelet tropomyosin chain. In solutions containing 150 mM KCl and 5 mM MgCl2, addition of actin at up to a sixfold molar excess over AD-P-TM caused both the fluorescence emission intensities and fluorescence polarization values of samples to increase. In the presence of actin, the wavelength of maximal emission was shifted to shorter values by about 5 to 7 nm. These changes indicate that actin does bind to AD-P-TM and that the binding affects the environment of the label, both by making it more hydrophobic and by reducing the freedom of the label to tumble in solution.     

Enhancer effect of fluorescein on the luminol–H2O2–horseradish peroxidase chemiluminescence: energy transfer process

The chemiluminescence of the luminol–H₂O₂–horseradish peroxidase system is increased by fluorescein. Fluorescein produces an enhancement of the luminol chemiluminescence similar to that of phenolphthalein, by an energy transfer process from luminol to fluorescein. The maximum intesity and the total chemiluminescence emission (between 380 and 580 nm) of luminol with fluorescein was more than three times greater than without fluorescein; however, the emission duration was shorter. The emission spectra in the presence of fluorescein had two maxima (425 and 535 nm) and the enhancement was dependent on pH and fluorescein concentration. A mechanism is proposed to explain these effects. © 1997 John Wiley & Sons, Ltd.     

Polarized fluorescence of aggregated bacteriochlorophyll c and baseplate bacteriochlorophyll a in single chlorosomes isolated from Chloroflexus aurantiacus

The polarization anisotropy of fluorescence from single chlorosomes isolated from a green filamentous bacterium, Chloroflexus aurantiacus, was measured using a confocal laser microscope at 13 K. Each single chlorosome that is floating in a frozen solvent exhibited strong polarization anisotropy of fluorescence. We calculated the degrees of fluorescence polarization for 51 floating single chlorosomes. The value ranged from 0.1 to 0.76 for the BChl-c aggregate in the core chlorosomes and from 0 to 0.4 for the energy acceptor BChl-a in the baseplate protein in the outer membrane. The shifts in polarization angles between the two emission bands were distributed over all the possible values with a sharp peak around 90 degrees , suggesting the perpendicular orientation between the transition dipoles of the fluorescence emission from the BChl-c aggregate and that from BChl-a. A simulation assuming a random orientation of chlorosomes reproduced the experimental results exactly. The analysis further indicated the appreciable contribution of the transition dipole of BChl-c that has an orientation perpendicular to the major polarization axis in each chlorosome. Small values of the degrees of polarization implied the BChl-a transition dipole to be somewhat tilted with respect to the normal of the cytoplasmic membrane to which chlorosomes are attached. These conclusions can be obtained only by observing the fluorescence of single chlorosomes.     

The respiratory chain of Paramecium tetraurelia in wild type and the mutant Cl1. I. Spectral properties and redox potentials.

1. Purified mitochondria have been prepared from wild type Paramecium tetraurelia and from the mutant Cl1 which lacks cytochrome aa3. Both mitochondrial preparations are characterized by cyanide insensitivity. Their spectral properties and their redox potentials have been studied. 2. Difference spectra (dithionite reduced minus oxidized) of mitochondria from wild type P. tetraurelia at 77 K revealed the alpha peaks of b-type cytochrome (s) at 553 and 557 nm, of c-type cytochrome at 549 nm and a-type cytochrome at 608 nm. Two alpha peaks at 549 and 545 nm could be distinguished in the isolated cytochrome c at 77 K. After cytochrome c extraction from wild type mitochondria, a new peak at 551 nm was unmasked, probably belonging to cytochdrome c1. The a-type cytochrome was characterized by a split Soret band with maxima at 441 and 450 nm. The mitochondria of the mutant Cl1 in exponential phase of growth differed from the wild type mitochondria in that cytochrome aa3 was absent while twice the quantity of cytochrome b was present. In stationary phase, mitochondria of the mutant were characterized by a new absorption peak at 590 nm. 3. Cytochrome aa3 was present at a concentration of 0.3 nmol/mg protein in wild type mitochondria and ubiquinone at a concentration of 8 nmol/mg protein both in mitochondria of the wild type and the mutant Cl1. Cytochrome aa3 was more susceptible to heat than cytochromes b and c,c1.     

Possible involvement of the lipid-peroxidation product 4-hydroxynonenal in the formation of fluorescent chromolipids.

The effects of the lipid-peroxidation product 4-hydroxynonenal on the formation of fluorescent chromolipids from microsomes, mitochondria and phospholipids were studied. Incubation of freshly prepared rat liver microsomes or mitochondria with 4-hydroxynonenal results in a slow formation of a fluorophore with an excitation maximum at 360 nm and an emission maximum at 430 nm. The rate and extent of the development of the 430 nm fluorescence can be significantly enhanced by ADP-iron (Fe3+). With microsomes, yet not with mitochondria. NADPH has a catalytic effect similar to that of ADP-iron. Fluorescent chromolipids with maximum excitation and emission at 360/430 nm are also formed during the NADPH-linked ADP-iron-stimulated lipid peroxidation. Phosphatidylethanolamine and phosphatidylserine react with 4-hydroxynonenal revealing a fluorophore with the same spectral characteristics as that obtained in the microsomal and mitochondrial system. The findings suggest that the fluorescent chromolipids formed by lipid peroxidation are not derived from malonaldehyde, but are formed from 4-hydroxynonenal or similar reactive aldehydes via a NADPH and/or ADP-iron-catalysed reaction with phosphatidylethanolamine and phosphatidylserine contained in the membrane.     

Flow system fluorescence polarization measurements on fluorescein diacetate-stained EL4 cells.

We have adapted a multiparameter cell sorter to measure the distribution of fluorescence polarization in cell populations. Measurements carried out on EL4 cells show that the percent polarization of fluorescein fluorescence decreases with increasing fluorescence intensity. This inverse relationship between polarization and intensity is shown both within the cell population and by the average values of the two quantities during both the increase and decrease of fluorescence intensity. The quantitative relation between intensity and polarization is different in hypertonic than in isotonic media. These results suggest that polarization measurements carried out at a fixed time after incubation of cells with fluorescein diacetate, which is converted to fluorescein within the cells, may depend in part on the rate of fluorescein accumulation, and that agents that have been reported to change the polarization of fluorescein in living cells may do so by changing the kinetics of fluorescein accumulation.     

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.     

Identification of two macrophage populations by flow cytometry monitoring of oxidative burst and phagocytic functions

Two populations of phagocytic cells from trehalose dimycolate-elicited mouse peritoneal cells are demonstrated by flow cytofluorometry, using two fluorescent probes excited at the same wavelength (488 nm). Liposomes containing diethylenetriaminepentaacetate daunorubicin conjugate (maximum emission wavelength: 590 nm) allow the discrimination of phagocytes and non-phagocytic cells. Among the phagocytes, an activated population is revealed by a cell-associated fluorescence of the oxidation product of dichlorofluorescein diacetate (maximum emission wavelength: 520 nm).     

USE OF FLUORESCENCE POLARIZATION DETECTION FOR THE MEASUREMENT OF FLUOPEPTIDE™ BINDING TO G PROTEIN-COUPLED RECEPTORS

ABSTRACT

G protein-coupled receptors (GPCRs) represent the single largest molecular target of therapeutic drugs currently on the market, and are also the most common target in high throughput screening assays designed to identify potential new drug candidates. A large percentage of these assays are now formatted as radioligand binding assays. Fluorescence polarization ligand binding assays can offer a non-rad alternative to radioligand binding assays. In addition, fluorescence polarization assays are a homogenous format that is easy to automate for high throughput screening. We have developed a series of peptide ligands labeled with the fluorescent dye BODIPY® TMR whose binding to GPCRs can be detected using fluorescence polarization methodology. BODIPY® TMR has advantages over the more commonly used fluorescein dye in high throughput screening (HTS) assays due to the fact that its excitation and emission spectra are red-shifted approximately 50 nm relative to fluorescein. Assays based on BODIPY® TMR ligands are therefore less susceptible to interference from tissue auto-fluorescence in the assay matrix, or the effects of colored or fluorescent compounds in the screening libraries. A series of BODIPY® TMR labeled peptides have been prepared that bind to a range of GPCRs including melanin concentrating hormone, bradykinin, and melanocortin receptors. Conditions have been optimized in order to utilize a comparable amount of receptor membrane preparation as is used in a radioligand binding assay. The assays are formatted in 384-well microplates with a standard volume of 40 µL. We have compared the assays across the different fluorescence polarization (FP) readers available to determine the parameters for each instrument necessary to achieve the required precision.     

Use of fluorescence polarization detection for the measurement of fluopeptidetm binding to G protein-coupled receptors

G protein-coupled receptors (GPCRs) represent the single largest molecular target of therapeutic drugs currently on the market, and are also the most common target in high throughput screening assays designed to identify potential new drug candidates. A large percentage of these assays are now formatted as radioligand binding assays. Fluorescence polarization ligand binding assays can offer a non-rad alternative to radioligand binding assays. In addition, fluorescence polarization assays are a homogenous format that is easy to automate for high throughput screening. We have developed a series of peptide ligands labeled with the fluorescent dye BODIPY TMR whose binding to GPCRs can be detected using fluorescence polarization methodology. BODIPY TMR has advantages over the more commonly used fluorescein dye in high throughput screening (HTS) assays due to the fact that its excitation and emission spectra are red-shifted approximately 50 nm relative to fluorescein. Assays based on BODIPY TMR ligands are therefore less susceptible to interference from tissue auto-fluorescence in the assay matrix, or the effects of colored or fluorescent compounds in the screening libraries. A series of BODIPY TMR labeled peptides have been prepared that bind to a range of GPCRs including melanin concentrating hormone, bradykinin, and melanocortin receptors. Conditions have been optimized in order to utilize a comparable amount of receptor membrane preparation as is used in a radioligand binding assay. The assays are formatted in 384-well microplates with a standard volume of 40 microL. We have compared the assays across the different fluorescence polarization (FP) readers available to determine the parameters for each instrument necessary to achieve the required precision.     

Polyvinyl pyrrolidone capped fluorescent anthracene nanoparticles for sensing fluorescein sodium in aqueous solution and analytical application for ophthalmic samples

Based on the known complexation ability between polyvinyl pyrrolidone (PVP) and fluorescein sodium (FL Na⁺), fluorescent PVP capped anthracene nanoparticles (PVP‐ANPs) were prepared using a reprecipitation method for detection of fluorescein in aqueous solution using the fluorescence resonance energy transfer (FRET) approach. A dynamic light scattering histogram of PVP‐ANPs showed narrower particle size distribution and the average particle size was 15 nm. The aggregation‐induced enhanced emission (AIEE) of PVP‐ANPs was red shifted from its monomer by 1087.22 cm^?1. The maximum emission was seen to occur at 420 nm. The presence of FL Na⁺ in the vicinity of PVP‐ANPs quenched the fluorescence of PVP‐ANPs because of its adsorption on the surface of PVP‐ANPs in aqueous suspension. The FL Na⁺ and PVP‐ANPs were brought close enough, typically to 7.89 nm, which was less than the distance of 10 nm that is required between the energy donor–acceptor molecule for efficient FRET. The quenching results fit into the Stern–Volmer relationship even at temperatures greater than ambient temperatures. The thermodynamic parameters determined from FRET results helped to propose binding mechanisms involving hydrophobic and electrostatic molecular interaction. The fluorescence quenching results were used further to develop an analytical method for estimation of fluorescein sodium from ophthalmic samples available commercially in the market. Copyright © 2015 John Wiley & Sons, Ltd.     

Rhodamine immunohistofluorescence applied to plant tissue.

Tissue slices from the roots and seeds of sanifoin (Onobrychis viciifolia, Scop.) exhibit bright autofluorescence when illuminated with blue (495 nm) light. This autofluorescence is indistinguishable from the fluorescence emission of fluorescein, the commonly used fluorochrome in immunohistochemical staining procedures. Rhodamine isothiocyanate, when coupled to immunoglobulin, and excited with green light at 546 nm, exhibits a reddish-orange fluorescence with an emission maximum at 590 nm. Plant tissue has little or no autofluorescence when illuminated at this wavelength and viewed with a 580 nm barrier filter. Therefore, use of rhodamine for immunohistochemical localization in plant tissue avoids interpretative complications due to inherent autofluorescence.     

Changes in the chlorophyll fluorescence characteristics of chloroplasts from intact pumpkin cotyledons,caused by organ excision and kinetin treatment

The chlorophyll (Chl) fluorescence emission as well as excitation and polarization characteristics of chloroplasts from intact cotyledons were determined in pumpkin seedlings after removal of one cotyledon (co-cotyledon) or apical bud or primary root, or after kinetin treatment of derooted seedlings. Qualitatively, the fluorescence emission and excitation spectra of chloroplasts were similar. The fluorescence emission spectra showed a maximum at 685 (F685) and a hump at 735 nm (F735), whereas the excitation spectra showed peaks at 439, 471, 485, and 676 nm. The fluorescence intensities at F685 and F735 differed in various groups of seedlings, as indicated by changes in their ratios. Similarly, the ratios of 471/439, 485/439, and 676/439 nm were also different. Variability in the Chl fluorescence intensity values and the fluorescence polarization of chloroplasts prepared from various seedling types may suggest a different degree of binding between the pigment complexes and light-harvesting Chl-protein (LHCP), resulting in different rates of photoexcitation energy loss in the form of fluorescence emission. Kinetin treatment improved the coupling of pigment complexes with reaction centre, as indicated by low polarization values in derooted and kinetin-treated seedlings, which suggests the development of a suntype chloroplast.     

Spectroscopic studies on origination of the peak at 730 nm in delayed fluorescence of chloroplasts.

The origination of the peak at 730 nm in the delayed fluorescence (DF) spectrum of chloroplasts was studied using various optical analysis methods. The DF spectrum showed that the main emission peak was at about 685 nm, with a small shoulder at 730 nm when the chloroplast concentration was < 7.8 microg/mL. The intensity of the peak at 685 nm decreased, while the intensity of the peak at 730 nm increased, when the chloroplast concentrations were increased from 7.8 to 31.2 microg/mL. With the concentration increasing, the peak at 730 nm became dominant while the peak at 685 nm finally disappeared. The DF decay kinetic curves showed that the intensity of the peak at 730 nm decayed as the same speed as the intensity of the peak at 685 nm during the entire relaxation process (0.5-30.5 s). With the excitation wavelength at 685 nm, the emission intensity was stronger in the excitation spectrum at 730 nm. The absorption spectrum demonstrated that the ratio A(685):A(730) remained almost constant when the chloroplast concentration increased. The results suggest that the peak at 730 nm appearing in DF is mainly contributed by the fluorescence of photosystem I (PSI), generated by the re-absorption of 685 nm band DF.     

Luminescence excitation spectra reveal low-lying excited states in stacked adenine bases

Luminescence emission, polarization, and excitation spectra of polyadenylic acid (poly(A)) have been studied in room-temperature aqueous solution (pH 8). The temperature dependence of the luminescence of poly(A) at two different excitation wavelengths in the range 10-70 degrees C has also been studied and compared with that of adenosine 5'-monophosphate (AMP). It has been found that the luminescence excitation spectrum and the polarization curve of poly(A) solution reveal a low-intensity electronic transition at about 320 nm which is red-shifted by approximately 0.9 eV from the maximum of the absorption spectrum at 260 nm. A model of two luminescent stacked forms is suggested. The difference in the ground state levels of these two stacked forms obtained from the temperature dependencies of the emissions is insignificant ( approximately 1 kcal/mol). This means a lowering of the excited state of the stacked form with the 320 nm/420 nm absorption/emission bands by approximately 0.9 eV as compared to the main form with the 260 nm/400 nm absorption/emission bands. The low-lying excited states suggest the stronger electronic coupling of the bases in a certain stacked form. It is proposed that such clusters of the stacked bases could provide the wire-like conductivity in the short segments of DNA.