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PubMed2001

Fluorescence lifetime heterogeneity in aggregates of LHCII revealed by time-resolved microscopy.

Two-photon excitation, time-resolved fluorescence microscopy was used to investigate the fluorescence quenching mechanisms in aggregates of light-harvesting chlorophyll a/b pigment protein complexes of photosystem II from green plants (LHCII). Time-gated microscopy images show the presence of large heterogeneity in fluorescence lifetimes not only for different LHCII aggregates, but also within a single aggregate. Thus, the fluorescence decay traces obtained from macroscopic measurements reflect an average over a large distribution of local fluorescence kinetics. This opens the possibility to resolve spatially different structural/functional units in chloroplasts and other heterogeneous photosynthetic systems in vivo, and gives the opportunity to investigate individually the excited states dynamics of each unit. We show that the lifetime distribution is sensitive to the concentration of quenchers contained in the system. Triplets, which are generated at high pulse repetition rates of excitation (>1 MHz), preferentially quench domains with initially shorter fluorescence lifetimes. This proves our previous prediction from singlet-singlet annihilation investigations (Barzda, V., V. Gulbinas, R. Kananavicius, V. Cervinskas, H. van Amerongen, R. van Grondelle, and L. Valkunas. 2001. Biophys. J. 80:2409-2421) that shorter fluorescence lifetimes originate from larger domains in LHCII aggregates. We found that singlet-singlet annihilation has a strong effect in time-resolved fluorescence microscopy of connective systems and has to be taken into consideration. Despite that, clear differences in fluorescence decays can be detected that can also qualitatively be understood.

Fluorescence↗
PubMed2002

The depth of porphyrin in a membrane and the membrane's physical properties affect the photosensitizing efficiency.

Photosensitized biological processes, as applied in photodynamic therapy, are based on light-triggered generation of molecular singlet oxygen by a membrane-residing sensitizer. Most of the sensitizers currently used are hydrophobic or amphiphilic porphyrins and their analogs. The possible activity of the short-lived singlet oxygen is limited to the time it is diffusing in the membrane, before it emerges into the aqueous environment. In this paper we demonstrate the enhancement of the photosensitization process that is obtained by newly synthesized protoporphyrin derivatives, which insert their tetrapyrrole chromophore deeper into the lipid bilayer of liposomes. The insertion was measured by fluorescence quenching by iodide and the photosensitization efficiency was measured with 9,10-dimethylanthracene, a fluorescent chemical target for singlet oxygen. We also show that when the bilayer undergoes a melting phase transition, or when it is fluidized by benzyl alcohol, the sensitization efficiency decreases because of the enhanced diffusion of singlet oxygen. The addition of cholesterol or of dimyristoyl phosphatydilcholine to the bilayer moves the porphyrin deeper into the bilayer; however, the ensuing effect on the sensitization efficiency is different in these two cases. These results could possibly define an additional criterion for the choice and design of hydrophobic, membrane-bound photosensitizers.

Cell Membrane↗
PubMed1977

Exciton annihilation in the two photosystems in chloroplasts at 100 degrees K.

The fluorescence yield (F) of spinach chloroplasts at 100 degrees K measured at 735 nm (photosystem I fluorescence-F 735) and at 685 nm (photosystem II fluorescence-F 685) has been determined with different modes of laser excitation. The modes of excitation included a single picosecond pulse, sequences of picosecond pulses (4, 22, and 300 pulses spaced 5 ns apart) and a single nonmode-locked 2-mus pulse (MP mode). The F 735/F 685 intensity ratios decrease from 1.62 to 0.61 when a single picosecond pulse (or low-power continuous helium-neon laser) is replaced by excitation with the 300-ps pulse train (PPT mode) or MP mode. In the PPT mode of excitation, the 735-nm fluorescence band is quenched by a factor of 45 as the intensity is increased from 10(15) to 10(18) photons/cm(2) per pulse train and the 685-nm fluorescence is quenched by a factor of 10. In the MP mode, the quenching factors are 25 and 7, respectively, in the same intensity range. Fluorescence quantum yield measurements with different picosecond pulse sequences indicate that relatively long-lived quenching species are operative, which survive from one picosecond pulse to another within the pulse train. The excitonic processes possible in the photosynthetic units are discussed in detail. The differences in the quenching factors between the MP and PPT modes of excitation are attributed to singlet-singlet annihilation, possible when picosecond pulses are utilized, but minimized in the MP mode of excitation. The long-lived quenchers are identified as triplets and/or bulk chlorophyll ions formed by singlet-singlet annihilation. The preferential quenching in photosystem I is attributed to triplet excitons. The influence of heating effects, photochemistry, bleaching, and two-photon processes is also considered and is shown to be negligible.

Chloroplasts↗
PubMed1996

Pigment-pigment interactions and energy transfer in the antenna complex of the photosynthetic bacterium Rhodopseudomonas acidophila.

BACKGROUND: Photosynthesis starts with the absorption of solar radiation by antenna pigment molecules. In purple bacteria these chromophores, (bacteriochlorophyll a and carotenoid) are embedded in the membrane; they are non-covalently bound to apoproteins which have the ability to modulate the chromophores' absorbing characteristics. The first structure of the bacterial antenna complex from Rhodopseudomonas acidophila, strain 10050, shows a ring of nonameric symmetry. Two concentric cylinders of apoproteins enclose the pigment molecules. The current resolution of the structure, to 2.5 A, allows us to begin to explore the mechanism of energy transfer among these pigments. RESULTS: The mechanism of energy transfer, from the short- to long-wavelength-absorbing pigments, is largely determined by the relative distances and orientations of the chromophores. In this paper we provide evidence that energy transfer between the B800 and B850 bacteriochlorophylls is largely via Förster induced dipole-dipole resonance. Strong Coulombic (exciton) coupling among the 18 short distanced chromophores in the B850 macrocycle is promoted by good alignment of the Qy dipoles. Singlet-singlet energy transfer from carotenoid to the B800 macrocycle appears to be minimal, with most of the energy transfer going to B850. The higher energy state of both chromophores dominates in more complex situations. CONCLUSIONS: The structure of the antenna complex not only shows Nature at its most aesthetic but also illustrates how clever and efficient the energy transfer mechanism has become, with singlet-singlet excitation being passed smoothly down the spectral gradient to the reaction centre.

Bacterial Proteins↗
PubMed2000

Electronic energy transfer involving carotenoid pigments in chlorosomes of two green bacteria: Chlorobium tepidum and Cholroflexus aurantiacus.

Electronic energy transfer processes in chlorosomes isolated from the green sulphur bacterium Chlorobium tepidum and from the green filamentous bacterium Chloroflexus aurantiacus have been investigated. Steady-state fluorescence excitation spectra and time-resolved triplet-minus-singlet (TmS) spectra, recorded at ambient temperature and under non-reducing or reducing conditions, are reported. The carotenoid (Car) pigments in both species transfer their singlet excitation to bacteriochlorophyll c (BChlc) with an efficiency which is high (between 0.5 and 0.8) but smaller than unity; BChlc and bacteriochlorophyll a (BChla) transfer their triplet excitation to the Car's with nearly 100% efficiency. The lifetime of the Car triplet states is approximately 3 micros, appreciably shorter than that of the Car triplets in the light-harvesting complex II (LHCII) in green plants and in other antenna systems. In both types of chlorosomes the yield of BChlc triplets (as judged from the yield of the Car triplets) remains insensitive to the redox conditions. In notable contrast the yield of BChlc singlet emission falls, upon a change from reducing to non-reducing conditions, by factors of 4 and 35 in Cfx. aurantiacus and Cb. tepidum, respectively. It is possible to account for these observations if one postulates that the bulk of the BChlc triplets originate either from a large BChlc pool which is essentially non-fluorescent and non-responsive to changes in the redox conditions, or as a result of a process which quenches BChlc singlet excitation and becomes more efficient under non-reducing conditions. In chlorosomes from Cfx. aurantiacus whose Car content is lowered, by hexane extraction, to 10% of the original value, nearly one-third of the photogenerated BChlc triplets still end up on the residual Car pigments, which is taken as evidence of BChlc-to-BChlc migration of triplet excitation; the BChlc triplets which escape rapid static quenching contribute a depletion signal at the long-wavelength edge of the Qy absorption band, indicating the existence of at least two pools of BChlc.

Carotenoids↗
PubMed2003

Photostability of luminescent ruthenium(II) complexes in polymers and in solution.

The effects of oxygen on the photochemical properties of ruthenium(II) complexes in solution and in polymers are reported. In solution, the complex is actually protected from decomposition by the presence of oxygen as a result of deactivation of the complex by oxygen quenching before it can undergo ligand loss by monomolecular dissociation; however, in polymers, the presence of oxygen increases photochemical decomposition. Singlet molecular oxygen, a product of the oxygen quenching process, may attack the ground state complex or triplet oxygen may directly attack the excited state of the complex. Both mechanisms may be involved in the photodestruction of the complex. The role of oxygen in the photodecomposition was examined by monitoring the photochemical decomposition of various complexes of different singlet oxygen reactivity, as well as absorption and mass spectroscopy studies. It is suggested that in polymers, unlike in solutions, the newly formed reactive singlet oxygen is not able to diffuse away from the complex. The singlet oxygen, trapped in close proximity to the metal complex, has an enhanced opportunity to attack it. This cage effect is supported by studies using tris(1,10-phenanthroline)ruthenium(II) in poly(ethylene glycol) of increasing molecular weight to create an increasingly constraining cage around the complex. Increased poly(ethylene glycol) molecular weight leads to increased oxygen attack of the complex, supporting the cage effect.

Journal Article↗
PubMed2005

Energy dissipation in multichromophoric single dendrimers.

Single-molecule spectroscopy of well-chosen dendritic multichromophoric systems allows investigation of fundamental photophysical processes such as energy or electron transfer in much greater detail than the respective ensemble measurements. In dendrimers with multiple chromophores, energy hopping and transfer to the chromophore with the energetically lowest S(1) state was observed. If more than one chromophore is in an excited state in one molecule, annihilation, either singlet-triplet or singlet-singlet, can occur. In the latter case, a higher singlet state is populated opening new deactivation pathways. In the presence of an electron donor, reversible electron transfer could be observed, and the rate constants of forward and backward electron transfer were established. The value of these rate constants fluctuates time-correlated with the rotational motion of the dendrimer arms and the mobility of the embedding matrix.

Dendrimers↗
PubMed1995

Determination of the metal ion separation and energies of the three lowest electronic states of dimanganese (II,II) complexes and enzymes: catalase and liver arginase.

The dimanganese (II,II) catalase from Thermus thermophilus, MnCat(II,II), arginase from rat liver, Arg(II,II), and several dimanganese(II,II) compounds, LMn2XY2, which are functional catalase mimics, all possess a pair of coupled Mn(II) ions in their catalytic sites. For each of these, we have measured by EPR spectroscopy the relative energies separating the three lowest electronic states (singlet, triplet, and quintet), described a general method for extracting the individual spectra for these states by multicomponent analysis, and determined the Mn-Mn separation. The triplet-singlet and quintet-singlet energy gaps were modeled well by fitting the temperature dependence of the EPR intensities to a Boltzmann expression for a pair of Mn(II) ions coupled by isotropic Heisenberg spin exchange (-2JS1S2). This dependence indicates diamagnetic ground states with delta E10 (cm-1) = magnitude of 2J = 4 and 11.2 cm-1 for Arg-(II,II)(+borate) and MnCat(II,II)(phosphate), respectively. This large difference in magnitude of 2J reflects either a difference in the bridging ligands or, possibly, a weaker ligand field (larger ionization potential) for the Mn(II) ions in arginase. In n-butanol/CH2Cl2 the triplet-singlet energy gaps for [LMn2(CH3CO2)](C1O4)2 (1), [LMn2(CH3CO2)3] (2), and [LMn2Cl3] (3), where HL = N,N,N',N'-tetrakis(2-methylenebenzimidazole)-1,3-diaminopropan+ ++-2-ol, are 23-24 cm-1. Comparison of the Heisenberg exchange interaction constants for more than 30 dimanganese(II,II) complexes suggests a possible bridging structure of (mu-OH)(mu-carboxylate)1-2 for MnCat(II,II), while the 3-fold weaker coupling in Arg(II,II) suggests mu-aqua in place of mu-hydroxide. EPR spectra of both the triplet and quintet electronic states were extracted and found to exhibit zero-field splittings (ZFS) and resolved 55Mn hyperfine splittings indicating spin-coupled Mn2-(II,II) species. The major ZFS interaction could be attributed to the magnetic dipole-dipole interaction between the Mn(II) ions. A linear correlation is observed between the crystallographically determined Mn-Mn distance and the ZFS of the quintet state (D2) for five dimanganese pairs for which both data sets are available. Using this correlation, the Mn-Mn distance in Arg(II,II) is predicted to be 3.36-3.57 A for the native enzyme (multiple forms) and 3.59 A for MnCat(II,II)(phosphate). Addition of the inhibitor borate to Arg(II,II) simplifies the ZFS, indicative of conversion to a single species with mean Mn-Mn separation of 3.50 A. The second metal ion in dinuclear complexes possessing a shared bridging ligand has been shown to attenuate the strength of the mu-ligand field potential, as monitored by the strength of the single ion ZFS.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗
PubMed1991

Determination of rates and yields of interchromophore (folate----flavin) energy transfer and intermolecular (flavin----DNA) electron transfer in Escherichia coli photolyase by time-resolved fluorescence and absorption spectroscopy.

Escherichia coli DNA photolyase, which photorepairs cyclobutane pyrimidine dimers, contains two chromophore cofactors, 1,5-dihydroflavin adenine dinucleotide (FADH2) and 5,10-methenyltetrahydrofolate (MTHF). Previous work has shown that MTHF is the primary photoreceptor which transfers energy to the FADH2 cofactor; the FADH2 singlet excited state then repairs the photodimer by electron transfer. In this study, we have determined the rate constants for these photophysical processes by time-resolved fluorescence and absorption spectroscopy. From time-resolved fluorescence, we find that energy transfer from MTHF to FADH2 and FADH degrees occurs at rates of 4.6 x 10(9) and 3.0 x 10(10) s-1, respectively, and electron transfer from FADH2 to a pyrimidine dimer occurs at a rate of 5.5 x 10(9) s-1. Using Förster theory for long-range energy transfer and assuming K2 = 2/3, the interchromophore distances were estimated to be 22 A in the case of the MTHF-FADH2 pair and 21 A for the MTHF-FADH degrees pair. Picosecond absorption spectroscopy identified an MTHF single state which decays to yield the first excited singlet state of FADH2. The lifetimes of MTHF and FADH2 singlets and the rates of interchromophore energy transfer, as well as the rate of electron transfer from FADH2 to DNA measured by time-resolved fluorescence, were in excellent agreement with the values obtained by picosecond laser flash photolysis. Similarly, fluorescence or absorption lifetime studies of the folate-depleted enzyme with and without photodimer suggest that FADH2, in its singlet excited state, transfers an electron to the dimer with 89% efficiency. The distance between FADH2 and the photodimer was calculated to be ca. 14 A.

Apoenzymes↗
PubMed1994

Product binding to the alpha-carboxyl subsite results in a conformational change at the active site of O-acetylserine sulfhydrylase-A: evidence from fluorescence spectroscopy.

The intrinsic fluorescence of the pyridoxal 5'-phosphate (PLP) enzyme O-acetylserine sulfhydrylase-A (OASS-A) was studied in order to gain insight into the structural basis for binding of substrates and products and for catalysis. Excitation of OASS-A with 298-nm light gives an emission spectrum with two maxima, 337 and 498 nm. OASS-A has two tryptophan residues, and the 337-nm maximum indicates that at least one of these is exposed somewhat to aqueous solvent. The 498-nm emission observed is due to fluorescence of the PLP Schiff base. Some of this long-wavelength fluorescence is likely due to direct excitation by incident radiation. However, the concomitant quenching of 340-nm emission and the enhancement of 498-nm emission observed upon reconstitution of apoenzyme with PLP support the conclusion that some of the long-wavelength emission is due to singlet-singlet transfer from at least one tryptophan residue to the PLP Schiff base. Enhancement of 498-nm fluorescence by either of the products, acetate or cysteine, of the enzymatic reaction without a quenching of 337-nm fluorescence is consistent with triplet-singlet transfer from one or both of the tryptophan residues to the PLP Schiff base. This would require a rigid environment for the tryptophan donor when the product is bound. However, a conformational change which affected principally the environment of the PLP Schiff base, resulting in a longer lifetime of its excited singlet state, would also increase the intensity of the 498-nm emission. Enhancement of OASS-A long-wavelength fluorescence by each product requires the unprotonated form of a different group on enzyme. Enhancement by acetate binding requires the unprotonated form of an enzyme group with a pK of 7 and is insensitive to substitution on the methyl group. L-Cysteine binding enhances 498-nm fluorescence when a group with a pK of 8 is unprotonated, and substitution at the thiol or the methylene bridge does not affect the enhancement elicited. Binding of L-cysteine to free enzyme (E) likely results in the formation of the external Schiff base accompanied by a conformational change giving fluorescence enhancement. The carboxylate moiety of acetate likely binds to the alpha-carboxylate subsite for amino acid reactants such as L-cysteine, resulting in a conformational change in the internal Schiff base and giving rise to the observed fluorescence enhancement. Data are interpreted in terms of the mechanism of OASS-A.

Acetates↗
PubMed1991

Effect of flavin structure and redox state on catalysis by and flavin-pterin energy transfer in Escherichia coli DNA photolyase.

5-DeazaFAD bound to a hydrophobic site in apophotolyase and formed a stable reconstituted enzyme, similar to that observed with FAD. Although stoichiometric incorporation was observed, the flavin ring modification in 1-deazaFAD interfered with normal binding, decreased protein stability, and prevented formation of a stable flavin radical, unlike that observed with FAD. The results suggest that an important hydrogen bond is formed between the protein and N (1) in FAD, but not N (5), and that there is sufficient space at the normal flavin binding site near N (5) to accommodate an additional hydrogen but not near N (1). Catalytic activity was observed with enzyme containing 5-deazaFADH2 (42% of native enzyme) or 1-deazaFADH2 (11% of native enzyme) as its only chromophore, but no activity was observed with the corresponding oxidized flavins, similar to that observed with FAD and consistent with a mechanism where dimer cleavage is initiated by electron donation from excited reduced flavin to substrate. The protein environment in photolyase selectively enhanced photochemical reactivity in the fully reduced state, as evidenced by comparison with results obtained in model studies with the corresponding free flavins. Phosphorescence was observed with free or photolyase-bound 5-deazaFADH2, providing the first example of a flavin that exhibits phosphorescence in the fully reduced state. Formation of an enzyme-substrate complex resulted in a nearly identical extent of quenching of 5-deazaFADH2 phosphorescence (85.1%) and fluorescence (87.5%). The data are consistent with a mechanism involving exclusive reaction of substrate with the excited singlet state of 5-deazaFADH2, analogous to that proposed for FADH2 in native enzyme. Direct evidence for singlet-singlet energy transfer from enzyme-bound 5-deazaFADH2 to 5,10-CH(+)-H4folate was provided by the fact that pterin fluorescence was observed upon excitation of 5-deazaFADH2, accompanied by a decrease in 5-deazaFADH2 fluorescence. On the other hand, the fluorescence of enzyme-bound pterin was quenched by 5-deazaFADox, consistent with energy transfer from pterin to 5-deazaFADox. In each case, the spectral properties of the chromophores were consistent with the observed direction of energy transfer and indicated that transfer in the opposite direction was energetically unlikely. Unlike 5-deazaFAD, energy transfer from pterin to FAD is energetically feasible with FADH2 or FADox. The results indicate that the direction of flavin-pterin energy transfer at the active site of photolyase can be manipulated by changes in the flavin ring or redox state which alter the energy level of the flavin singlet.

Deoxyribodipyrimidine Photo-Lyase↗
PubMed1983

Total internal reflection fluorescence study of energy transfer in surface-adsorbed and dissolved bovine serum albumin.

A simple adaptation of a commercial spectrofluorometer allows selective excitation of fluorescent biomolecules adsorbed to a solid surface while they are in equilibrium with a bulk solution. As a demonstration of this technique, we have detected a change in the effective singlet-singlet energy transfer in fluorescence-labeled bovine serum albumin (BSA) upon adsorption to a fused silica surface. The technique combines total internal reflection fluorescence excitation of surface-adsorbed BSA with a fluorescence spectroscopic examination of energy transfer between two different fluorophores that are covalently bound to amino groups in each BSA molecule. Two donor--acceptor pairs were used, 4-chloro-7-nitro-2,1,3-benzoxadiazole-rhodamine and dansyl-eosin. For studies of surface-adsorbed BSA, we constructed a device in which the excitation light of a standard fluorescence spectrometer totally internally reflects from a surface at which adsorbed BSA is in equilibrium with the bulk solution. A shallow evanescent wave is created, which excites fluorescence from only those BSA molecules in close proximity to the surface. Spectral examination shows significantly less effective singlet-singlet energy transfer from the donor to the acceptor in surface-adsorbed BSA relative to that in native bulk-dissolved BSA. Under appropriate and reasonable assumptions, the energy transfer change between native and adsorbed states of fluorescent BSA can be interpreted as a conformational change of BSA upon adsorption.

Adsorption↗
PubMed1988

Accessibilities of the sulfhydryl groups of native and photooxidized lens crystallins: a fluorescence lifetime and quenching study.

Fluorescence lifetime and acrylamide quenching studies on the N-(iodoacetyl)-N'-(5-sulfo-1-naphthyl)ethylenediamine (1,5-IAEDANS)-labeled sulfhydryl groups of bovine lens alpha-, beta H-, and gamma-crystallins were carried out to characterize the microenvironment of the sulfhydryls and changes produced by singlet oxygen mediated photooxidation. For the untreated proteins, the lifetimes of the major decay component of the fluorescence-labeled crystallins were 15.2, 14.4, and 13.0 ns, and the quenching rate constant, kq, values were 16.6 x 10(7), 26.9 x 10(7), and 32.7 x 10(7) M-1 s-1 for alpha-, beta H-, and gamma-crystallins, respectively. The results indicate that as the polarity of the sulfhydryl site increased (i.e., its lifetime decreased), its accessibility to collisional quenching by acrylamide also increased. The minor decay component of the fluorescence label was not significantly quenched by acrylamide for all three classes of crystallins. When the proteins were irradiated in the presence of methylene blue, in a system generating singlet oxygen, the kq value for acrylamide quenching of the major decay component of alpha-crystallin decreased to zero, while its lifetime decreased to 6 ns. Neither the lifetime nor the kq of alpha-crystallin recovered completely in the presence of the singlet oxygen quencher sodium azide. Light-induced binding of the photosensitizer methylene blue to the crystallins was observed by absorption spectroscopy. The bound photosensitizer partially quenches the fluorescence lifetime of the N-acetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine (AEDANS) label in irradiated alpha-crystallin. Further decrease in the lifetime occurs as a result of the singlet oxygen mediated conformational change. The results suggest that the fluorescence lifetime of the AEDANS is fully quenched in the irradiated alpha-crystallin and there is no further quenching by acrylamide. An increase in the fraction of the minor component of beta H-crystallin which was inaccessible to acrylamide quenching was observed after irradiation. There was no effect of irradiation on the kq for acrylamide quenching of the major component of the decay of AEDANS bound to beta H- or gamma-crystallins. Static quenching was found to contribute significantly to the steady-state quenching plots of the polar sulfhydryl sites of irradiated alpha-crystallin and of untreated and irradiated beta H- and gamma-crystallins, but it had no detectable role in the case of untreated alpha-crystallin. Fluorescence anisotropy of the AEDANS label bound to the crystallins was higher in the irradiated crystallins as compared with the controls.

Acrylamide↗
PubMed1981

Fluorescence studies of the beta-adrenergic receptor topology.

The nature of the propranolol binding site of the beta-adrenergic receptor has been examined by utilizing the intrinsic fluorescence of propranolol as a probe. Additionally, the spatial relationship between the propranolol binding site and membrane tryptophan has been examined by utilizing I-quenching of intrinsic tryptophan fluorescence, chemical modification of membrane tryptophan, and singlet-singlet energy transfer between membrane-bound propranolol and tryptophan. Propranolol, at concentrations consistent with specific beta-receptor binding, protected approximately 42% of the membrane tryptophan fluorescence from I-quenching. Further, in the presence of propranolol, the apparent quenching constant (kq) was altered from 3.6 to 21.8 M-1. Reaction of the membrane fragments with 2-hydroxy-5-nitrobenzyl bromide (Koshland's reagent I) in the presence and absence of propranolol indicated that low concentrations of propranolol protected approximately 45% of the membrane tryptophan from the reagent. The singlet-singlet energy transfer from tryptophan to propranolol was determined by sensitized emission. The distance between these two species was found to be less than 20 A. These results have been interpreted to indicate that propranolol, when bound to the beta-adrenergic receptor, is situated such that its naphthyl moiety is inserted into a tryptophan-rich hydrophobic pocket of the receptor.

Animals↗
PubMed2002

High-field EPR study of tyrosyl radicals in prostaglandin H(2) synthase-1.

Various tyrosyl radicals generated by reaction of both native and indomethacin-inhibited ovine prostaglandin H synthase-1 with ethyl hydrogen peroxide were examined by using high-field/high-frequency EPR spectroscopy. The spectra for the initially formed tyrosyl radical commonly referred to as the "wide-doublet" species and the subsequent "wide-singlet" species as well as the indomethacin-inhibited "narrow-singlet" species were recorded at several frequencies and analyzed. For all three species, the g-values were distributed. In the case of the wide doublet, the high-field EPR spectra indicated that dominant hyperfine coupling was likely to be also distributed. The g(x)-values for all three radicals were found to be consistent with a hydrogen-bonded tyrosyl radical. In the case of the wide-doublet species, this finding is consistent with the known position of the radical and the crystallographic structure and is in contradiction with recent ENDOR measurements. The high-field EPR observations are consistent with the model in which the tyrosyl phenyl ring rotates with respect to both the protein backbone and the putative hydrogen bond donor during evolution from the wide-doublet to the wide-singlet species. The high-field spectra also indicated that the g-values of two types of narrow-singlet species, self-inactivated and indomethacin-inhibited, were likely to be different, raising the possibility that the site of the radical is different or that the binding of the inhibitor perturbs the electrostatic environment of the radical. The 130 GHz pulsed EPR experiments performed on the wide-doublet species indicated that the possible interaction between the radical and the oxoferryl heme species was very weak.

Animals↗
PubMedDate not supplied

Antibody-targeted photolysis: in vitro immunological, photophysical, and cytotoxic properties of monoclonal antibody-dextran-Sn(IV) chlorin e6 immunoconjugates.

A set of anti-melanoma immunoconjugates were prepared which contained chlorin e6: antibody molar ratios of 18.9:1, 11.2:1, 6.8:1, and 1.7:1. All immunoconjugates retained antigen binding activity regardless of the chromophore:antibody substitution ratio that was attained. In contrast, the ground-state absorption spectra of the immunoconjugates showed features which appeared to be dependent on the chromophore:antibody molar ratio. In addition, the quantum yield of singlet oxygen generated by the conjugated chromophores was observed to be significantly less than that observed with the unbound dye. Time-resolved absorbance spectroscopy of the chromophore excited triplet state indicated that the loss of singlet oxygen quantum yield resulted from diminished chromophore triplet yield. Analysis of data obtained from in vitro photolysis of target melanoma cells, in combination with that obtained from the immunochemical and photochemical studies, indicates that the observed immunoconjugate phototoxicity can be reasonably quantitatively represented by (1) the ability of the immunoconjugate to bind SK-MEL-2 cell surface antigen, (2) the amount of chromophore localized at the target cells by immunoconjugate binding, (3) the delivered dose of light at 634 nm, and (4) the singlet oxygen quantum yield of the antibody-bound photosensitizer. Though these data argue strongly for photolysis by the cumulative dosage of singlet oxygen at the cell membrane, nonetheless, the concurrent photoinduced release of other cytotoxic agents should not be ruled out.

Antibodies, Monoclonal↗
PubMed2000

2,5-Dimethylfuran (DMFu): An Internal Standard for the "Traceless" Quantitation of Unknown Samples via (1)H NMR.

The use of 2,5-dimethylfuran (DMFu) as an internal standard for the quantitation of unknown samples by (1)H NMR is described. DMFu was selected based upon its low chemical reactivity, good solubility in standard NMR solvents, appropriate volatility (bp 92 degrees C), and the chemical shifts of its two singlets (5.80 and 2.20 ppm). In particular, the widely separated singlets of DMFu offer two advantages over more traditional "single peak" internal standards (e.g., hexamethyldisiloxane): (1) they reduce the possibility for overlap between analyte and internal standard signals; and (2) they enable the chemist to assess the accuracy of integration (and ergo, the quantitation) by calculating the ratio of the two singlets and comparing the observed ratio to the theoretical value. Our experiments have shown that the precision of the ratio of DMFu singlets strongly correlates to the precision of sample quantitation, an observation which greatly simplifies the assessment of the quality of the quantitation. Utilizing this technique, we have developed straightforward conditions for (1)H NMR experiments which consistently provide quantitative results with less than 5.0% error.

Journal Article↗
PubMed2001

Photophysics of pyridylporphyrin Ru(II) adducts: heavy-atom effects and intramolecular decay pathways.

Eight adducts between different pyridylporphyrins and ruthenium complexes, MPyP[RuCl(2)(DMSO)(2)(CO)], c-DPyP[RuCl(2)(DMSO)(2)(CO)](2), TrPyP[RuCl(2)(DMSO)(2)(CO)](3), TPyP[RuCl(2)(DMSO)(2)(CO)](4), (MPyP)(2)[RuCl(2)(DMSO)(2)], [c-DPyP[RuCl(2)(DMSO)(2)]](2), MPyP[RuCl(2)(CO)(3)], and [c-DPyP[RuCl(2)(CO)(2)]](2), have been investigated. The results show that in all the adducts the porphyrin singlet is quenched, to a greater or lesser extent, relative to the parent-free molecule. This study provides insight into the mechanisms of singlet quenching in the adducts. Two mechanisms for singlet quenching, both related to the "heavy-atom effect" of the ruthenium center and experimentally distinguishable by transient spectroscopy, are examined. Enhanced intersystem crossing within the porphyrin chromophore is demonstrated for the series of adducts MPyP[RuCl(2)(DMSO)(2)(CO)], c-DPyP[RuCl(2)(DMSO)(2)(CO)](2), TrPyP[RuCl(2)(DMSO)(2)(CO)](3), and TPyP[RuCl(2)(DMSO)(2)(CO)](4), where a nice correlation is observed between the magnitude of the effect and the number of ruthenium centers attached to the pyridylporphyrin chromophore. Singlet-triplet energy transfer from the pyridylporphyrin chromophore to the ruthenium center(s) is an additional efficient quenching channel for adducts containing ruthenium centers with weak field ligands and low triplet energies, such as (MPyP)(2)[RuCl(2)(DMSO)(2)] and [c-DPyP[RuCl(2)(DMSO)(2)]](2).

Chemical Phenomena↗