Isomerization of Diphenyl Polyenes

We describe an unusual temperature dependence of 1,8-diphenyl-1,3,5,7-octatetraene absorption in poly(vinyl alcohol) films. Upon heating above 80 °C, the optical density (in the long wavelength region) of this compound increases rapidly. A sample heated to 150 °C has a nearly twenty times higher optical density than a non-heated sample. This effect is not reversible: Once the sample is heated it retains its absorbance on cooling to room temperature. In our opinion, the effect has its origin in changes of the chromophore molecules from cis to trans conformation at the high temperature. Possible applications of these unique material properties should be improved temperature sensors, optical data storage, non-developed high resolution photography or typing, etc.

Proton and iron ion observations from a solid-state microdosimeter

The tissue equivalent proportional counter (TEPC) that utilises a gas cavity has been the standard to obtain microdosimetric observations. An alternative is the solid-state microdosimeter that replaces the gas with a solid-state detector with microscopic sensitive volumes. Here, we describe the development of two versions of a personal solid-state microdosimeter for space exploration applications and give test results for iron and proton beams with comparisons to TEPC measurements and Geant4 radiation transport code simulations. In addition, we describe and provide test results of an optical technique to carry out an end-to-end system test and calibration of a silicon solid-state microdosimeter. This technique eliminates the need for an ionising radiation source with its attendant issues on use and transportation and provides an advantage over the TEPC.

Microdosemeter instrument (MIDN) for assessing risk in space

Radiation in space generally produces higher dose rates than that on the Earth's surface, and contributions from primary galactic and solar events increase with altitude within the magnetosphere. Presently, no personnel monitor is available to astronauts for real-time monitoring of dose, radiation quality and regulatory risk. This group is developing a prototypic instrument for use in an unknown, time-varying radiation field. This microdosemeter-dosemeter nucleon instrument is for use in a spacesuit, spacecraft, remote rover and other applications. It provides absorbed dose, dose rate and dose equivalent in real time so that action can be taken to reduce exposure. Such a system has applications in health physics, anti-terrorism and radiation-hardening of electronics as well. The space system is described and results of ground-based studies are presented and compared with predictions of transport codes. An early prototype in 2007 was successfully launched, the only solid-state microdosemeter to have flown in space.

End-to-end system test for solid-state microdosemeters

The gold standard in microdosemeters has been the tissue equivalent proportional counter (TEPC) that utilises a gas cavity. An alternative is the solid-state microdosemeter that replaces the gas with a condensed phase (silicon) detector with microscopic sensitive volumes. Calibrations of gas and solid-state microdosemeters are generally carried out using radiation sources built into the detector that impose restrictions on their handling, transportation and licensing in accordance with the regulations from international, national and local nuclear regulatory bodies. Here a novel method is presented for carrying out a calibration and end-to-end system test of a microdosemeter using low-energy photons as the initiating energy source, thus obviating the need for a regulated ionising radiation source. This technique may be utilised to calibrate both a solid-state microdosemeter and, with modification, a TEPC with the higher average ionisation energy of a gas.

Thermodynamics and dynamics of histidine-binding protein, the water-soluble receptor of histidine permease. Implications for the transport of high and low affinity ligands

The bacterial histidine permease is a model system for ABC transporters (traffic ATPases). The water-soluble receptor of this permease, HisJ, binds L-histidine and L-arginine (tightly) and L-lysine and L-ornithine (less tightly) in the periplasm, interacts with the membrane-bound complex (HisQMP2) and induces its ATPase activity, which results in ligand translocation. HisJ is a two-domain protein; in the absence of ligand, the cleft between two domains is open and binding of substrate stabilizes the closed conformation. Surprisingly, various liganded HisJ forms display substantial differences in their physicochemical characteristics and capacity to induce the ATPase. This is due to either different effects of the individual ligands on the respective closed structures, or to different equilibria being reached for each ligand between the open liganded form and the closed liganded form [Wolf, A. , Lee, K.C., Kirsch, J.F. & Ames, G.F.-L. (1996) J. Biol. Chem. 271, 21243-21250]. In this work, time-resolved measurements of the decay of intrinsic HisJ fluorescence and of the decay of the anisotropy of the fluorescence, as well as the analysis of the steady-state near UV CD and fluorescence spectra, rule out the model in which the differences between liganded complexes reflect different equilibria. The decay of the anisotropy of the fluorescence shows that liganded complexes differ dramatically in their large-scale conformational dynamics. Differential scanning calorimetry (DSC) curves for the HisJ thermal unfolding are well described by a scheme of equilibrium two-state unfolding of two independent domains, which can be ascribed to the two-domain structure of HisJ. This is true both for apo-HisJ at various pH values, and for HisJ in the presence of its ligands at varying concentrations, at pH 8.3. The DSC and structural data suggest that all ligands interact more extensively with the larger domain. A qualitative model for the HisJ conformational dynamics employing the idea of a twisting movement of the domains is proposed, which explains the difference in the efficacy of the ATPase induction by the various liganded HisJ forms.

beta-glycosidase from the hyperthermophilic archaeon Sulfolobus solfataricus: structure and activity in the presence of alcohols

beta-Glycosidase from the extreme thermophilic archaeon Sulfolobus solfataricus is a tetrameric protein with a molecular mass of 240 kDa, stable in the presence of detergents, and with a maximal activity at temperatures above 95 degrees C. Understanding the structure-activity relationships of the enzyme under different conditions is of fundamental importance for both theoretical and applicative purposes. In this paper we report the effect of methanol, ethanol, 1-propanol, and 1-butanol on the activity of S. solfataricus beta-glycosidase expressed in Escherichia coli. The alcohols stimulated the enzyme activity, with 1-butanol producing its maximum effect at a lower concentration than the other alcohols. The structure of the enzyme was studied in the presence of 1-butanol by circular dichroism, and Fourier-transform infrared and fluorescence spectroscopies. Circular dichroism and steady-state fluorescence measurements revealed that at low temperatures the presence of the alcohol produced no significant changes in the tertiary structure of the enzyme. However, time-resolved fluorescence data showed that the alcohol modifies the protein microenvironment, leading to a more flexible enzyme structure, which is probably responsible for the enhanced enzymatic activity.

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.

Bilin organization in cryptomonad biliproteins

The bilin organization of three cryptomonad biliproteins (phycocyanins 612 and 645 and phycoerythrin 545) was examined in detail. Two others (phycocyanin 630 and phycoerythrin 566) were studied less extensively. Phycocyanin 645 and phycoerythrin 545 were suggested to have one bilin in each monomeric (alphabeta) unit of the dimer (alpha2beta2) isolated from the others, and the remaining six bilins may be in pairs. One pair was found across the monomer-monomer interface of the protein dimer, and two identical pairs were proposed to be within the monomer protein units. For phycocyanin 612, a major surprise was that a pair of bilins was apparently not found across the monomer-monomer interface, but the remaining bilins were distributed as in the other two cryptomonad proteins. The effect of temperature on the CD spectra of phycocyainin 612 demonstrated that two of the bands (one positive and one negative) behaved identically, which is required if they are coupled. The two lowest-energy CD bands of phycocyanin 612 originated from paired bilins, and the two higher-energy bands were from more isolated bilins. The paired bilins within the protein monomers contained the lowest-energy transition for these biliproteins. Using the bilins as naturally occurring reporter groups, phycocyanin 612 was shown to undergo a reversible change in tertiary structure at 40 degrees C. Protein monomers were shown to be functioning biliproteins. A hypothesis is that the coupled pair of bilins within the monomeric units offers important advantages for efficient energy migration, and other bilins transfer energy to this pair, extending the wavelength range or efficiency of light absorption.

Distances between the paclitaxel, colchicine, and exchangeable GTP binding sites on tubulin

Distances between the paclitaxel, colchicine, and exchangeable GTP binding sites on tubulin polymers have been probed using fluorescence spectroscopy. Techniques for measuring fluorescence resonance energy transfer (FRET) between fluorescent or chromophoric ligands for each binding site were employed. 2-Debenzoyl-2-(m-aminobenzoyl)paclitaxel (2-AB-PT) was the fluorophore ligand for the paclitaxel binding site; thiocolchicine, allocolchicine, and MDL 27048 were probes for the colchicine site, and 2'(or 3')-O-(trinitrophenyl)guanosine 5'-triphosphate (TNP-GTP) was the fluorophore ligand for the exchangeable GTP site. The distance between the colchicine and paclitaxel binding sites was determined with two different acceptor ligands in the colchicine site. An average distance distribution of 17 A was found in both cases. Energy transfer between 2-AB-PT bound to the paclitaxel site and TNP-GTP (acceptor) bound to the exchangeable GTP site was observed in the polymer. The average distance distribution between the fluorophores was 16.0 A, but the half-width of the distribution was large (17.9 A), which indicates that energy transfer between more than one donor-acceptor pair occurred in the system. One interpretation of this result is that 2-AB-PT serves as an energy transfer donor for two GTP sites, one contained on the same subunit and one on an adjacent protofilament. No FRET was observed between ligands bound to the colchicine and exchangeable GTP sites, indicating that the result of colchicine binding on the GTP region of beta-tubulin is a long range, allosteric effect. The results from these experiments are interpreted in terms of known structural features of microtubules.

Phycoerythrin 545: monomers, energy migration, bilin topography, and monomer/dimer equilibrium

Phycoerythrin 545 was isolated having an alpha2beta2 (dimer) protein structure at pH 6.0 and 2 g/L protein concentration with eight bilin chromophores. Monomers (alphabeta) were produced by lowering the protein concentration to 0.15 g/L and the pH to 4.5. Dimer dissociation was monitored by dynamic light scattering and gel-filtration column chromatography. Monomers were stable and had bilin optical spectra different from the alpha2beta2 dimers, although they have very similar protein secondary structures. The optical spectra of phycoerythrin 545 showed four types of behavior with temperature: 10-20 degrees C, dimers; 40-50 degrees C, dimers/monomers; 60 degrees C, nearly fully disordered; 70 degrees C, disordered alpha and beta polypeptides. At 40 degrees C, the protein dissociated partially to monomer, which could be totally reversed to dimers at 20-25 degrees C. The visible circular dichroism difference spectrum for the protein dimers minus monomers exhibited positive and negative bands--such spectra may indicate exciton splitting between closely-spaced bilins. Circular dichroism also revealed a spectrum suggesting exciton coupling for the second excited state of the bilins. Ultrafast fluorescence using a two-photon method showed the fastest time for protein dimers to be 2. 4 ps and monomers had a 39-ps lifetime. Phycocyanin 645 was found to have a 550-fs lifetime.

Two-photon excitation of ethidium bromide labeled DNA

We examined the steady state and time-resolved emission of DNA stained with ethidium bromide (EB) when excited with 90 fs pulses from a mode-locked titanium sapphire laser. Over the wavelength range from 840 to 880 nm EB-DNA was found to display two-photon excitation, with a cross-section near 7 x 10(-50) cm4s/photon. Frequency-domain intensity decay measurements revealed similar multi-exponential intensity decays for one- and two-photon excitation. Time-resolved anisotropy decay measurements revealed similar correlation times, but different amplitudes as has been observed previously for two- versus one-photon excitation. These results indicate that two-photon excitation of EB-DNA can be accomplished with the fundamental output of a Ti:sapphire laser without obvious heating or perturbation of the DNA.

Time-resolved fluorescence spectroscopy and imaging of DNA labeled with DAPI and Hoechst 33342 using three-photon excitation

We examined the fluorescence spectral properties of the DNA stains DAPI (4',6-diamidino-2-phenylindole, hydrochloride) and Hoechst 33342 (bis-benzimide, or 2,5'-bi'1H-benzimidazole2'-(4-ethoxyphenyl)-5-(4-methyl-1-piperazi nyl)) with two-photon (2h nu) and three-photon (3h nu) excitation using femtosecond pulses from a Ti:sapphire laser from 830 to 885 nm. The mode of excitation of DAPI bound to DNA changed from two-photon at 830 nm to three-photon at 885 nm. In contrast, Hoechst 33342 displayed only two-photon excitation from 830 to 885 nm. DAPI-DNA displayed the same emission spectra and decay times for 2h nu and 3h nu excitation. Hoechst 33342-DNA displayed the same intensity decay for excitation at 830 and 885 nm. Both probes displayed higher anisotropies for multiphoton excitation as compared to one-photon excitation with ultraviolet wavelengths, and DAPI-DNA displays a higher anisotropy for 3h nu at 885 nm than for 2h nu at 830 nm. We used 970-nm excitation of DAPI-stained chromosomes to obtain the first three-dimensional images with three-photon excitation. Three-photon excitation of DAPI-stained chromosomes at 970 nm was demonstrated by the power dependence in the fluorescence microscope.

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.

Fluorescence of reduced nicotinamides using one- and two-photon excitation

We examined the steady-state and time-resolved emission of NADH and NAMH resulting from one-photon and two-photon excitation. Similar emission spectra were observed for both modes of excitation. The fundamental anisotropy of NADH is near 0.54 for two-photon excitation from 690 to 740 nm, which is 46% higher than the value of 0.37 observed for one-photon excitation. This observation of a higher anisotropy with two-photon excitation was consistent with INDO/SDCI calculations of the one- and two-photon transitions. Minor differences in the multi-exponential decays of NADH were observed for one- and two-photon excitation, but presently available resolution does not allow us to conclude the decays are distinct. NADH-LADH-IBA complex formation led to an order of magnitude larger of the average lifetimes of NADH fluorescence resulting from one- and two-photon excitation. Fluorescence intensity and fluorescence anisotropy decays of NADH was double-exponential for both modes of excitation and show that the observed heterogeneity of the fluorescence decay kinetics of reduced nicotinamides arises from the inherent photoprocess of the dihydronicotinamide chromophore and not due to any intramolecular interactions with adenine part of NADH. Such interactions are responsible for the depolarization of NADH fluorescence observed for excitation wavelength below 300 nm for OPE and 600 nm for TPE, respectively. NADH displays a low cross-section for two-photon excitation which suggests that fluorescence from NADH will be moderately difficult to observe with two-photon fluorescence microscopy, and may not interfere with observations of TPIF of other extrinsic probes used to label cells.

Fluorescence detection of the anticancer drug topotecan in plasma and whole blood by two-photon excitation

The anticancer drug topotecan was detected in human plasma and whole blood using two-photon excitation at 730 or 820 nm. These wavelengths are longer than the main absorption bands of hemoglobin. Two-photon excitation of topotecan was demonstrated by a quadratic dependence of the emission intensity on the incident power, compared to a linear dependence for one-photon excitation at 410 nm. The observed emission centered at 525 nm was shown to be topotecan from the similarity of the emission spectrum and decay times observed for one-photon and two-photon excitation. Topotecan was detected at concentrations as low as 0.05 and 1 microM in plasma and whole blood, respectively. Since skin blood and tissues are translucent at long wavelengths, these results suggest the possibility of homogeneous or noninvasive clinical sensing with two-photon excitation.

Two-color two-photon excitation of fluorescence

We report the observation of two-photon excitation of an organic fluorophore with two different wavelengths, a phenomenon we refer to as two-color two-photon (2C2P) excitation. Ultraviolet emission of p-terphenyl at 340 nm was observed when the sample was illuminated with both 375 and 750 nm pulses from a picosecond dye laser. The emission of p-terphenyl was about 100-fold and more than 1000-fold less for illumination at only 375 or 750 nm, respectively. Observation of the 2C2P signal required temporal and spatial overlap of the 375 and 750 nm pulses. The amplitude of the signal depended on the polarization of each beam. 2C2P excitation can have applications in fluorescence microscopy and elsewhere when spatially localized excitation is desirable.

The carbohydrate moieties of the beta-subunit of Na+, K(+)-ATPase: their lateral motions and proximity to the cardiac glycoside site

The beta-subunit associated with the catalytic (alpha) subunit of the mammalian Na+, K(+) -ATPase is a transmembrane glycoprotein with three extracellularly located N-glycosylation sites. Although beta appears to be essential for a functional enzyme, the role of beta and its sugars remains unknown. In these studies, steady-state and dynamic fluorescence measurements of the fluorophore lucifer yellow (LY) covalently linked to the carbohydrate chains of beta have demonstrated that the bound probes are highly solvent exposed but restricted in their diffusional motions. Furthermore, the probes' environments on beta were not altered by Na+ or K+ or ouabain-induced enzyme conformational changes, but both divalent cation and oligomycin addition evoked modest changes in LY fluorescence. Frequency domain measurements reflecting the Förster fluorescence energy transfer (FET) occurring between anthroylouabain (AO) bound to the cardiac glycoside receptor site on alpha and the carbohydrate-linked LY demonstrated their close proximity (18 A). Additional FET determinations made between LY as donor and erythrosin-5-isothiocyanate, covalently bound at the enzyme's putative ATP binding site domain, indicated that a distance of about 85 A separates these two regions and that this distance is reduced upon divalent cation binding and increased upon the Na+E1-->K+E2 conformational transition. These data suggest a model for the localization of the terminal moieties of the oligosaccharides that places them, on average, about 18 A from the AO binding site and this distance or less from the extracellular membrane surface.

Studies on the dissociation of cryptomonad biliproteins

The spectroscopic properties of two biliproteins, phycocyanin 645 and phycoerythrin 566, have been studied by treating the proteins with two different agents, NaSCN at pH 6.0, or pH 4.0 without NaSCN. For phycoerythrin 566, treatment with NaSCN revealed that the visible CD spectrum of its chromophores was separated into a pair of different spectra, and each of these spectra was observed as a negative and one or more positive bands. For phycocyanin 645, two negative CD bands have been observed previously, together with two or more positive bands, in the dimer (alpha 2 beta 2) state, and NaSCN treatment caused elimination of one of these negative bands. The dimer was stable at pH 6.0, but at pH 4.0 the spectra of phycocyanin 645 had one less negative band than those at pH 6.0. Chromatography demonstrated that phycocyanin 645 was a monomer (alpha beta) at pH 4.0. Monomers of cryptomonad biliproteins have never been observed before. Excitation at 514 nm, in picosecond time-resolved fluorescence studies, produced lifetimes of 11.0 and 45.2 ps for dimers and monomers, respectively. Excitation at 566 nm yielded times of 1.38 and 1.24 ps, for dimers and monomers, respectively. CD in the far UV showed that monomers and dimers had very similar secondary structures. These results have been used to test an hypothesis that proposed two types of exciton splitting among the chromophores of phycocyanin 645, and perhaps phycoerythrin 566 could also have this chromophore organization.

Fluorescence anisotropy of tyrosine using one-and two-photon excitation

We examined the emission spectra and steady-state anisotropy of tyrosyl fluorescence with two-photon excitation from 565 to 578 nm. The emission spectra of phenol and N-acetyl-L-tyrosinamide (NATyrA) were all the same for one-photon excitation (OPE) and two-photon excitation (TPE), and the tyrosine emission from ribonuclease A showed 10-nm shift to longer wavelengths with TPE. Surprisingly, the anisotropy of tyrosine, NATyrA and Leu5-enkephalin in frozen solution were near zero for TPE as compared to near 0.3 for OPE. Low values of the anisotropy near 0.05 were also found for phenol and ribonuclease A. A low anisotropy appears to be a basic characteristic of tyrosine or tyrosyl residues with two-photon excitation.

Reduced albumin binding promotes the stability and activity of topotecan in human blood

Topotecan, a semisynthetic water-soluble analogue of camptothecin, is the first topoisomerase I targeting anticancer agent to enter comparative phase III clinical trials. Here we elucidate the biophysical factors underlying the markedly improved bloodstream stability and cytotoxic activity of topotecan relative to camptothecin. Each agent contains an alpha-hydroxy-delta-lactone ring that hydrolyzes under physiological pH to yield a biologically-inactive carboxylate form. In human plasma, camptothecin lactone converts rapidly and completely to its carboxylate form due to a 200-fold binding preference by serum albumin (HSA) for the latter [Mi, Z., & Burke, T.G. (1994) Biochemistry 33, 10540-12545]. Time-resolved fluorescence anisotropy measurements reveal that neither topotecan lactone nor carboxylate associates with HSA, thereby resulting in a significantly higher level of lactone stability in plasma for topotecan (t1/2 = 23.1 min, percent lactone at equilibrium of 17.6) relative to camptothecin (t1/2 = 10.6 min, percent lactone at equilibrium of < 0.2). Moreover, studies with HL-60 human promyelocytic leukemia cells reveal that a physiologically-relevant level (40 mg/mL) of HSA dramatically attenuates the cytotoxic activity of camptothecin in excess of 2600-fold (for a 72 h exposure, the IC50 value of 1.5 nM in the absence of HSA increased to 4 microM in the presence of HSA). The activities of other clinically relevant anticancer analogues, 9-aminocamptothecin and SN-38, were also strongly modulated by the presence of 40 mg/mL HSA. In marked contrast, the presence of HSA effected no change on the cytotoxic activity of topotecan (IC50 = 12 nM both in the absence and in presence of HSA).(ABSTRACT TRUNCATED AT 250 WORDS)

Calcium-induced troponin flexibility revealed by distance distribution measurements between engineered sites

The contraction of vertebrate striated muscle is regulated by Ca2+ binding to troponin C (TnC). This causes conformational changes which alter the interaction of TnC with the inhibitory protein TnI and the tropomyosin-binding protein TnT. We have used the frequency domain method of fluorescence resonance energy transfer to measure TnT-TnC and TnT-TnI distances and distance distributions, in the presence of Ca2+, Mg2+, or EGTA, in TnC.TnI.TnT complexes. We reconstituted functional, ternary troponin complexes using the following recombinant subunits whose sequences were based on those of rabbit skeletal muscle: wild-type TnC; TnT25, a mutant C-terminal 25-kDa fragment of TnT containing a single Trp212 which was used as the sole donor for fluorescence energy transfer measurements; Trp-less TnI mutants which contained either no Cys or a single Cys at position 9, 96, or 117. Energy acceptor groups were introduced into TnC or TnI by labeling with dansyl aziridine or N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine. Our results indicate that the troponin complex is relatively rigid in relaxed muscle, but becomes much more flexible when Ca2+ binds to regulatory sites in TnC. This increased flexibility may be propagated to the whole thin filament, releasing the inhibition of actomyosin ATPase activity and allowing the muscle to contract. This is the first report of distance distribution measurements between troponin subunits.

Synthesis and interaction of fluorescent thapsigargin derivatives with the sarcoplasmic reticulum ATPase membrane-bound region

Fluorescent derivatives of thapsigargin (TG) were synthesized by replacing the C8-butanoyl chain with a dansyl (DTG) or eosin (ETG) moiety. DTG and ETG retain the inhibitory effect of TG on the sarcoplasmic reticulum (SR) ATPase, displaying a 2 and 10 microM Ki, respectively. Steady state and lifetime fluorescence measurements are consistent with energy transfer between tryptophanyl residues assigned to the ATPase membrane-bound region and DTG. This phenomenon exhibits saturation behavior, occurs in the presence of DTG concentrations producing ATPase inhibition, and is partially prevented by inhibitory concentrations of TG. Although long range conformational effects of TG binding affect the fluorescence properties of endogenous tryptophans as well as of a fluorescein 5'-isothiocyanate (FITC) label of the ATPase extramembranous region, no significant energy transfer was detected between DTG and the FITC label. It is concluded that the inhibitors partition within the membrane and the binding domain resides within or near the membrane-bound region of the ATPase.

Interactions between chlorophyll a and beta-carotene in nematic liquid crystals

Fluorescence lifetime in the ps range, polarized absorption, polarized fluorescence spectra and delayed luminescence time resolved spectra were measured for chlorophyll a solutions with and without beta-carotene addition in nematic liquid crystal. Photoacoustic spectra of the same samples at various frequencies of light modulation were also taken. The frequency dependence of the photoacoustic spectra suggests that part of the excitation is converted into heat in a slow process (with a decay time of the order of ms). The lifetime results suggest that at used concentration some aggregation of the chlorophyll a occurs. The chlorophyll a molecules interact strongly with the beta-carotene forming some nonfluorescent or weakly fluorescent aggregates characterized by having various thermal deactivation yields and orientations in anisotropic matrix when compared to those of separated pigments. It seems that the aggregated forms of the chlorophylls are partially disrupted as a result of the their interaction with the beta-carotene. Singlet excitation of beta-carotene is not transferred to the fluorescent form of chlorophyll a. Delayed (in microsecond time range) luminescence of chlorophyll a is quenched by beta-carotene. This luminescence is located in the same spectral region as prompt fluorescence. Interactions between chlorophyll a and beta-carotene depend on the degree of pigment orientation and their aggregation.

Metal-ligand complexes as a new class of long-lived fluorophores for protein hydrodynamics

We describe the use of asymmetric Ru-ligand complexes as a new class of luminescent probes that can be used to measure rotational motions of proteins. These complexes are known to display luminescent lifetimes ranging from 10 to 4000 ns. In this report, we show that the asymmetric complex Ru(bpy)2(dcbpy) (PF6)2 displays a high anisotropy value when excited in the long wavelength absorption band. For covalent linkage to proteins, we synthesized the N-hydroxy succinimide ester of this metal-ligand complex. To illustrate the usefulness of these probes, we describe the intensity and anisotropy decays of [Ru(bpy)2(dcbpy)] when covalently linked to human serum albumin, concanavalin A (ConA), human immunoglobulin G (IgG), and Ferritin, and measured in solutions of increased viscosity. These data demonstrate that the probes can be used to measure rotational motions on the 10 ns to 1.5 microseconds timescale, which so far has been inaccessible using luminescence methods. The present probe [Ru(bpy)2(dcbpy)] can be regarded as the first of a class of metal-ligand complexes, each with different chemical reactivity and spectral properties, for studies of macromolecular dynamics.

Intramolecular dynamics in the environment of the single tryptophan residue in staphylococcal nuclease

The dipole relaxational dynamics in the environment of a single tryptophan residue Trp-140 in staphylococcal nuclease was studied by time-resolved (multi-frequency phase-modulation) spectroscopy and selective red-edge excitation. The long-wavelength position of the fluorescence spectrum (at 343 nm) and the absence of red-edge excitation effects at 0 and 20 degrees C indicate that this residue is surrounded by very mobile protein groups which relax on the subnanosecond time scale. For these temperatures (0-20 degrees C) the steady-state emission spectra did not show the excitation-wavelength dependent shifts (red-edge effects) for excitation wavelengths from 295 to 308 nm; however, the anisotropy decay rate is slow (tens of nanoseconds). This suggests that the spectral relaxation is due to mobility of the surrounding groups rather than the motion of the tryptophan itself. The motions of the tryptophan surrounding are substantially retarded at reduced temperatures in viscous solvent (60% glycerol). The temperature dependence of the difference in position of fluorescence spectra at excitation wavelengths 295 and 305 nm demonstrate the existence of red-edge effect at sub-zero temperatures, reaching a maximum value at -50 degrees C, where the steady-state emission spectrum is shifted to 332 nm. The excitation and emission wavelength dependence of multi-frequency phase-modulation data at the half-transition point (-40 degrees C) demonstrates the existence of the nanosecond dipolar relaxations. At -40 degrees C the time-dependent spectral shift is close to monoexponential with the relaxation time of 1.4 ns.

Homogeneous model immunoassay of thyroxine by phase-modulation fluorescence spectroscopy

We describe a homogeneous competitive model immunoassay for determination of thyroxine by multifrequency phase-modulation fluorescence. Using a nonradiative energy transfer transduction mechanism, B-phycoerythrin conjugated to thyroxine is the energy donor and a carboxymethylindocyanine dye conjugated to anti-thyroxine antibody is the energy acceptor. Energy transfer from B-phycoerythrin to the acceptor results in a decreased lifetime and/or phase angle. The fluorescence lifetime change reflects the extent of energy transfer. In the competitive immunoassay format, the donor-thyroxine conjugate and an analytical sample of thyroxine compete for acceptor-antibody binding sites, resulting in a phase angle change which is dependent on the amount of thyroxine in the sample. Dose-response curves of phase angle versus thyroxine concentration are comparable to steady-state intensity curves. Since phase-modulation lifetime measurements are largely independent of total signal intensity, sources of optical interference are minimized. The potential for whole blood measurements exists since the energy transfer lifetime method can be extended to longer wavelengths.

Fluorescence study of a temperature-induced conversion from the "loose" to the "tight" binding form of membrane-bound cytochrome b5

Cytochrome b5 is a liver integral membrane protein that has now been expressed in, and isolated from, Escherichia coli. The structure-function relationships of the 43 amino acid membrane-binding domain (nonpolar peptide) have been examined in both native and mutant forms of the protein; in the latter, tryptophan residues at positions 108 and 112 were replaced by leucine. The temperature dependence of the fluorescence quantum yield of the Trp residues in the isolated membrane-binding domain was examined while the domain was bound to lipid vesicles. Both the lipid-bound mutant domain and lipid-bound native domain showed an irreversible increase in fluorescence above 50 degrees C. When the whole cytochrome b5 molecule, bound to lipid vesicles, was heated to this temperature, there was a conversion of the metastable, intermembrane-exchangeable ("loosely" bound), conformation to a final, virtually unexchangeable ("tightly" bound), conformation. It has been suggested previously that the protein exists in a "looped back" conformation and a "bilayer penetrating" conformation. Although the present studies are not designed to determine the absolute conformations of the loose and tight forms, the changes observed in steady-state and frequency-modulated fluorescence and the lack of change in depth of Trp 109 in the bilayer are consistent with a movement of the C-terminal segment from a looped back to a bilayer penetrating conformation as the tight form is generated.

Structural perturbation of the transmembrane region interferes with calcium binding by the Ca2+ transport ATPase

The Ca(2+)-ATPase of sarcoplasmic reticulum reacts with N-cyclohexyl-N'-(4-dimethylamino-1-naphthyl) carbodiimide (NCD4) yielding a fluorescence labeling that interferes with calcium binding to activating and transport sites of the enzyme and, thereby, with Ca(2+)-dependent ATPase activity. On the other hand, the catalytic site does not appear altered, as revealed by the normal occurrence of Ca(2+)-independent reactions, such as enzyme phosphorylation with Pi in the reverse direction of the catalytic cycle. This reaction is not inhibited by Ca2+ in the labeled enzyme, while it is inhibited in the native enzyme. The NCD4 reaction which is involved in functional inactivation occurs in the membrane-bound portion of the ATPase. Sodium dodecyl sulfate solubilization of hydrophobic peptides, electrophoresis, and microsequencing of transblotted electrophoretic bands revealed that the fluorescent NCD4 label resides in a segment of tryptic fragment A1, intervening between Glu231 and Glu309. This segment includes two transmembrane helices, and does not include the domain involved in the phosphoryl transfer reaction during catalytic activity. This specific labeling does not occur when the NCD4 derivatization procedure is carried out in the presence of Ca2+ concentrations that also prevent functional inactivation. Fluorescence characterization by steady state and intensity decay measurements shows only negligible energy transfer between the NCD4 label and fluorescein isothiocyanate label of Lys515, indicating that the NCD4 label is unlikely to reside within the extramembranous region of the ATPase. On the other hand, the fluorescence emission of intrinsic tryptophan residues clustered within or near the transmembrane region of the ATPase, is distinctly affected by NCD4 label specifically bound to the ATPase, and NCD4 label nonspecifically bound to the sarcoplasmic reticulum membrane. The combined sequencing and spectroscopic observations indicate that derivatization with NCD4 induces a perturbation within or near the transmembrane region of the ATPase (at a relatively large distance from the catalytic site) that interferes with specific calcium binding. This is in agreement with experiments (Clarke et al., 1989) demonstrating that mutations of any of six amino acids within the transmembrane region of the ATPase interfere with enzyme activation by Ca2+.

Conformational flexibility of the Cys 697-Cys 707 segment of myosin subfragment-1. Distance distributions by frequency-domain fluorometry

The separation between Cys 697 (SH1) and Cys 707 (SH2) of the heavy chain of myosin subfragment-1 was previously measured by fluorescence resonance energy transfer with a donor linked to SH1 and an acceptor to SH2. In the present study the distribution of the distances between the two thiols was recovered from frequency-domain fluorometry. In the native state and in the presence of ligands such as MgADP, pyrophosphate, orthovanadate (Vi) and actin, we found wide distributions of the separations between SH1 and SH2 (11-16 A) comparable to that found in the random-coil state (20 A). These results suggest that the SH1-SH2 segment has a high degree of conformational flexibility even in native S1. The flexibility is not much affected by the physiological state of S1. However, the ligands MgADP, Vi and MgADP + Vi decrease significantly the mean SH1-SH2 distance from 27 to 17 A with the effect of MgADP+ Vi being the most pronounced. The anisotropy decay of donor-labeled S1 is biphasic with two rotational correlation times. The long component is decreased by these ligands from 289 to 93 ns, suggesting a more compact symmetric structure of S1 in the presence of the ligands. The complex S1(MgADP)Vi has been shown to be a stable analogue of S1(MgADP)Pi, an unstable intermediate that is generated in the actomyosin ATPase cycle during muscle contraction. Since the power stroke of muscle is accompanied by release of Pi from S1(MgADP)Pi, the present results are consistent with a model in which force generation can be accompanied by transition of S1 from a highly symmetric or compact structure to a more extended structure.

Local phenomena and distribution of molecular species during the unfolding of heme-free myoglobin in the presence of GdnHCl and urea as seen by time-resolved fluorescence spectroscopy

We have used time-resolved fluorescence spectroscopy for following the unfolding of apomyoglobin in urea and guanidine hydrochloride (GdnHCl). The data have been compared with those obtained using classical techniques such as CD and steady-state emission spectroscopy. Both the average intensity of the lifetimes and the size of the librational cone of the fluorophores, as measured by time-resolved fluorescence, increased with denaturant concentration and their changes largely preceded the modifications detectable with CD and the shift of the maximum of emission spectra. The data indicate that the changes in the local environments of the tryptophans were completed when the global modification monitored by CD and the emission spectra was still minimal. This suggests that an initial event in the denaturation of apomyoglobin is localized at the tryptophan residues. The correlation times of native apomyoglobin showed the rotational diffusion characteristics of a rigid rotor. In 3.6 M GdnHCl and 7.5 M urea, where the secondary structure is practically absent, the correlation times of the two systems became very short, as expected from the motion of a flexible polymer. In GdnHCl, under conditions of partial unfolding, it was not possible to detect the presence of native totally folded molecular species.

Time-resolved emission spectra of hemoglobin on the picosecond time scale

We used front-face illumination to examine the steady-state and time-resolved emission from the intrinsic tryptophan emission of human hemoglobin (Hb). Experimental conditions were identified which eliminated all contributions of scattered light. The sensitivity obtained using front-face optics was adequate to allow measurement of the wavelength-dependent frequency response of the emission to 2 GHz. The intensity decays displayed pico- and nanosecond components in the emission at all wavelengths from 315 to 380 nm. The contribution of the picosecond component decreased from 72 to 37% over this range of wavelengths. Frequency-domain measurements were used to calculate the time-resolved emission spectra and decay-associated emission spectra. These spectra indicate that the picosecond components of the emission display maxima near 320 nm, whereas the nanosecond components are centered at longer wavelengths near 335 nm. The nanosecond components appear to be due to residual impurities which remain even in highly purified samples of Hb. However, we cannot eliminate the possibility that some of these components are due to Hb itself.

Resolution of the lifetimes and correlation times of the intrinsic tryptophan fluorescence of human hemoglobin solutions using 2 GHz frequency-domain fluorometry

We used 2 GHz harmonic content frequency-domain fluorescence to measure the intensity and the anisotropy decays from the intrinsic tryptophan fluorescence from human hemoglobin (Hb). The tryptophan intensity decays are dominated by a short-lived component which accounts for 35-60% of the total steady state intensity. The decay time of this short component varies from 9 to 27 ps and this component is sensitive to the ligation state of Hb. Our error analyses indicate the uncertainty is about +/- 3 ps. The intensity decays also show two longer lived components near 0.7 and 8 ns, which are probably due either to impurities or to Hb molecules in conformations which do not permit energy transfer. The anisotropy decays indicate the tryptophan residues in Hb are highly mobile, with apparent correlation times near 55 ps.