Delphine Onidas

Adenine, deoxyadenosine and deoxyadenosine 5'-monophosphate studied by femtosecond fluorescence upconversion spectroscopy

Abstract Aqueous solutions of adenine (A), deoxyadenosine (dA) and deoxyadenosine 5′-monophosphate (dAMP) were studied in room temperature by femtosecond fluorescence upconversion. The fluorescence decays cannot be described by single exponentials. They consist of an ultrafast component (230 fs for A, fs for dA and dAMP) and a slower one (8 ps for A, 0.5 ps for dA and dAMP). The slow component constitutes 95% of the total fluorescence (time-integrated) for the base while only 24% for the nucleoside or the nucleotide. The initial fluorescence anisotropy is 0.30±0.03 for A, 0.25±0.05 for dA and dAMP. The anisotropy of the A fluorescence partially decays during its lifetime due to rotational diffusion.

Electronic excited states responsible for dimer formation upon UV absorption directly by thymine strands: joint experimental and theoretical study.

The study addresses interconnected issues related to two major types of cycloadditions between adjacent thymines in DNA leading to cyclobutane dimers (T<>Ts) and (6-4) adducts. Experimental results are obtained for the single strand (dT)(20) by steady-state and time-resolved optical spectroscopy, as well as by HPLC coupled to mass spectrometry. Calculations are carried out for the dinucleoside monophosphate in water using the TD-M052X method and including the polarizable continuum model; the reliability of TD-M052X is checked against CASPT2 calculations regarding the behavior of two stacked thymines in the gas phase. It is shown that irradiation at the main absorption band leads to cyclobutane dimers (T<>Ts) and (6-4) adducts via different electronic excited states. T<>Ts are formed via (1)ππ* excitons; [2 + 2] dimerization proceeds along a barrierless path, in line with the constant quantum yield (0.05) with the irradiation wavelength, the contribution of the (3)ππ* state to this reaction being less than 10%. The formation of oxetane, the reaction intermediate leading to (6-4) adducts, occurs via charge transfer excited states involving two stacked thymines, whose fingerprint is detected in the fluorescence spectra; it involves an energy barrier explaining the important decrease in the quantum yield of (6-4) adducts with the irradiation wavelength.

Fluorescence of the DNA double helices (dAdT)n·(dAdT)n studied by femtosecond spectroscopy

Polymeric and oligomeric DNA helices, poly(dAdT).poly(dAdT) and (dAdT)(10).(dAdT)(10), composed of 200-400 and 20 adenine-thymine base pairs, respectively, are studied by fluorescence upconversion. Fluorescence decays, anisotropy decays and time-resolved spectra, obtained for this alternating base sequence, are compared with those determined previously for the homopolymeric sequence (dA)(n).(dT)(n). It is shown that identical fluorescence decays may correspond to quite different anisotropy decays and vice versa, both varying with the emission wavelength, the base sequence and the duplex size. Our observations cannot be explained in terms of monomer and excimer emission exclusively, as concluded in the past on the basis of steady-state measurements. Excitons also contribute to the fluorescence. These are rapidly trapped by excimers, characterized by long-lived weak emission.

Histidine is involved in coupling proton uptake to electron transfer in photosynthetic proteins.

In photosynthesis, the central step in transforming light energy into chemical energy is the coupling of light-induced electron transfer to proton uptake and release. Despite intense investigations of different photosynthetic protein complexes, including the photosystem II (PS II) in plants and the reaction center (RC) in bacteria, the molecular details of this fundamental process remain incompletely understood. In the RC of Rhodobacter (Rb.) sphaeroides, fast formation of the charge separated state, P(+)Q(A)(-), is followed by a slower electron transfer from the primary acceptor, Q(A), to the secondary acceptor, Q(B), and the uptake of a proton from the cytoplasm. The proton transfer to Q(B) takes place via a protonated water chain. Mutation of the amino acid AspL210 to Asn (L210DN mutant) near the entry of the proton pathway can disturb this water chain and consequently slow down proton uptake. Time-resolved step-scan Fourier transform infrared (FTIR) measurements revealed an intermediate X in the Q(A)(-)Q(B) to Q(A)Q(B)(-) transition. The nature of this transition remains a matter of debate. In this study, we investigated the role of the iron-histidine complex located between Q(A) and Q(B). We used time-resolved fast-scan FTIR spectroscopy to characterize the Rb. sphaeroides L210DN RC mutant marked with isotopically labeled histidine. FTIR marker bands of the intermediate X between 1120 cm(-1) and 1050 cm(-1) are assigned to histidine vibrations and indicate the protonation of a histidine, most likely HisL190, during the disappearance of the intermediate. Based on these results we propose a novel mechanism of the coupling of electron and proton transfer in photosynthesis.

Mutational control of bioenergetics of bacterial reaction center probed by delayed fluorescence

The free energy gap between the metastable charge separated state P(+)QA(-) and the excited bacteriochlorophyll dimer P* was measured by delayed fluorescence of the dimer in mutant reaction center proteins of the photosynthetic bacterium Rhodobacter sphaeroides. The mutations were engineered both at the donor (L131L, M160L, M197F and M202H) and acceptor (M265I and M234E) sides. While the donor side mutations changed systematically the number of H-bonds to P, the acceptor side mutations modified the energetics of QA by altering the van-der-Waals and electronic interactions (M265IT) and H-bond network to the acidic cluster around QB (M234EH, M234EL, M234EA and M234ER). All mutants decreased the free energy gap of the wild type RC (~890meV), i.e. destabilized the P(+)QA(-) charge pair by 60-110meV at pH8. Multiple modifications in the hydrogen bonding pattern to P resulted in systematic changes of the free energy gap. The destabilization showed no pH-dependence (M234 mutants) or slight increase (WT, donor-side mutants and M265IT above pH8) with average slope of 10-15meV/pH unit over the 6-10.5pH range. In wild type and donor-side mutants, the free energy change of the charge separation consisted of mainly enthalpic term but the acceptor side mutants showed increased entropic (even above that of enthalpic) contributions. This could include softening the structure of the iron ligand (M234EH) and the QA binding pocket (M265IT) and/or increase of the multiplicity of the electron transfer of charge separation in the acceptor side upon mutation.

Chloroform induces outstanding crystallization of poly(hydroxybutyrate) (PHB) vesicles within bacteria

AbstractPoly[(R)-3-hydroxyalkanoate]s or PHAs are aliphatic polyesters produced by numerous microorganisms. They are accumulated as energy and carbon reserve in the form of small intracellular vesicles. Poly[(R)-3-hydroxybutyrate] (PHB) is the most ubiquitous and simplest PHA. An atomic force microscope coupled with a tunable infrared laser (AFM-IR) was used to record highly spatially resolved infrared spectra of commercial purified PHB and native PHB within bacteria. For the first time, the crystallinity degree of native PHB within vesicle has been directly evaluated in situ without alteration due to the measure or extraction and purification steps of the polymer: native PHB is in crystalline state at 15% whereas crystallinity degree reaches 57% in commercial PHB. Chloroform addition on native PHB induces crystallization of the polymer within bacteria up to 60%. This possibility of probing and changing the physical state of polymer in situ could open alternative ways of production for PHB and others biopolymers. Graphical abstractAn atomic force microscope coupled with a tunable infrared laser (AFM-IR) has been used to record local infrared spectra of biopolymer PHB within bacteria. Deconvolution of those spectra has allowed to determine in situ the crystallinity degree of native PHB

Interaction between non-anionic phospholipids and cytochrome c induced by reactive oxygen species.

The oxidative interaction of cytochrome c (Cyt c) with liposomes of Palmitoyl Linoleyl Phosphatidyl Choline (PLPC) initiated by radio-induced free radicals was investigated. Results showed that the peroxidation of PLPC is decreased in the presence of Cyt c, meaning that this latter is the preferential target of hydroxyl radicals. In addition, when Cyt c was incubated with peroxidized PLPC, it was found to be able to decompose hydroperoxides of PLPC into hydroxides. The peroxidase activity of Cyt c proceeded via the opening of the tertiary structure of Cyt c, as suggested by the loss of the sixth coordination bond of the heme-iron. Even if it is known to preferentially interact with cardiolipin, this work shows that Cyt c is also able to interact with hydroperoxide species of non-anionic phospholipids.

Chapter 91 - Femtosecond fluorescence studies of DNA constitutents

To study the excited state one may use transient absorption or time-resolved fluorescence techniques. In both cases, DNA poses many problems. Its steady-state spectra are situated in the near ultraviolet spectral region, which is not easily accessible, by standard spectroscopic methods. Moreover, DNA and its constituents are characterized by extremely low fluorescence quantum yields ( −4 ) which renders fluorescence studies particularly difficult. This chapter describes the fluorescence upconversion set-up in more detail. Briefly, the third harmonic of a mode-locked Ti-sapphire laser (40 mW at 267 nm) is used as an excitation source. The fluorescence is collected by parabolic mirrors and focused into a 1 mm thick BBO type I crystal together with the residual beam of the fundamental radiation. The sum-frequency light thus generated is spectrally filtered by a double grating monochromator and detected by a photomultiplier running in photon counting mode. The apparatus function is determined by measuring the width of the dominant Raman line of water at 296 nm and is found to be around 450 fs (fwhm). Experimental data are analyzed by fitting with mono- or bi-exponential functions convoluted with a Gaussian apparatus response function.