Brevets |
Hocine Khemliche, P. R., Patrick Rousseau. (2012). Device and method for characterizing surfaces.
Résumé: A method of characterizing surfaces comprises the steps of:
directing a beam (2) of neutral atoms or molecules on a surface (3) for characterizing; and
detecting in position-sensitive manner the neutral atoms or molecules of said beam that have been diffused forwards by said surface (3) for characterizing;
the properties of said beam (2) being selected in such a manner that at least some of said neutral atoms or molecules that are diffused forwards are diffractive by said surface for characterizing.
A device for implementing such a method comprises means (1) for generating such a beam (2) of neutral atoms or molecules and position-sensitive detector means (4) for detecting the neutral atoms or molecules that are diffused forwards by said surface (3) for characterizing.
date de priorité: 7 juil. 2006
EP2044423A2, US20090250600, WO2008003865A2, WO2008003865A3
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Peer-reviewed Publications |
Alata, I., Broquier, M., Dedonder, C., Jouvet, C., & Marceca, E. (2012). Electronic excited states of protonated aromatic molecules: Protonated Fluorene. CHEMICAL PHYSICS, 393(1).
Résumé: The photo-fragmentation spectrum of protonated fluorene has been recorded in the visible spectral region, evidencing an absorption that appears largely red shifted in comparison to that of the neutral molecule fluorene. The spectrum shows two different vibrational progressions, separated by 0.19 eV. As in the case of protonated linear polycyclic aromatic hydrocarbons (PAHs), comparison of the measured spectra with ab initio calculations allows to associate the observed absorption shift with the charge transfer character of the excited state. The spectra can be properly simulated by geometry optimization of the ground and excited states, followed by Franck Condon analysis. The two vibrational bands progressions observed are assigned, with relatively good confidence, to the existence of two different conformers. (C) 2011 Elsevier B. V. All rights reserved.
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Alata, I., Omidyan, R., Broquier, M., Dedonder, C., & Jouvet, C. (2012). Protonated salicylaldehyde: Electronic properties. CHEMICAL PHYSICS, 399, 224–231.
Résumé: The excitation spectrum of protonated salicylaldehyde has been recorded in the 20,800-22,400 cm(-1) region (480-450 nm). The first excited state of protonated salicylaldehyde is a pi pi* state, largely red shifted as compared to the pi pi* transition of its neutral analogue. Like protonated benzaldehyde and in contrast to some other protonated aromatic molecules such as benzene or tryptophan in which the excited state dynamics is so fast that no vibrational structure can be observed, the vibrational bands are well resolved and assigned. This molecule has many low energy isomers and the simulations of the electronic spectrum via ab initio excited state optimizations and Franck-Condon calculations are precise enough to assign the observed electronic spectrum to one of the isomers. (C) 2011 Elsevier B.V. All rights reserved.
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Arabei, S. M., Galaup, J. - P., McCaffrey, J. G., Shafizadeh, N., & Crepin, C. (2012). Electronic spectroscopy, stimulated emission, and persistent spectral hole burning of cryogenic nitrogen matrices doped with tetrabenzoporphin. LOW TEMPERATURE PHYSICS, 38(8), 727–731.
Résumé: This paper deals with our on-going work on the electronic spectroscopy of tetrapyrrole molecules embedded in cryogenic hosts. Under nanosecond laser excitation of free-base tetrabenzoporphin molecules in a nitrogen matrix at 8 K, increasing laser pulse energy results in essential enhancement of the intensity of one or several vibronic emission lines in the fine-structure fluorescence spectrum. Some characteristics of stimulated radiation are realized in the observed intense monochromatic: radiation as a result of a transition from the purely electronic S-1 level to a vibrational sublevel of the S-0 state, corresponding to the excitation of C-C stretching vibrations of tetrapyrrole methane bridges. We also report on persistent spectral hole-burning effects. Hole and antihole formation analysis gives some insight on the photochemical properties of tetrabenzoporphin in a nitrogen matrix. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4746794]
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Atabek, O. (2012). Ultrafast intense laser induced molecular dissociation: Imaging and control. Balkan Physics Letters, 20, 37.
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Bailleux, S., Martin-Drumel, M. A., Margules, L., Pirali, O., Wlodarczak, G., Roy, P., Roueff, E., Gerin, M., Faure, A., & Hily-Blant, P. (2012). High-resolution terahertz spectroscopy of the (NH)-N-15 radical ((X)over-tilde (3)Sigma(-)). ASTRONOMY & ASTROPHYSICS, 538, A135.
Résumé: Context. High-resolution rotational spectroscopy of the imidogen radical has been limited to the (NH)-N-14 and (ND)-N-14 isotopologues. Imidogen is an important intermediate in the astronomical synthesis of ammonia. Recently, the N-14/N-15 isotopic ratio in ammonia has been obtained in cold, dense molecular clouds. Aims. We conducted a laboratory search for rotational transitions of (NH)-N-15 to investigate in more detail the N-14/N-15 ratio in the interstellar medium. Methods. (NH)-N-15 was generated in a positive column discharge in a flowing (NH3)-N-15 – He (SOLEIL synchrotron) or (NH3)-N-15 – Ar (PhLAM) mixture. High-resolution spectroscopic study of the (NH)-N-15 isotopologue of imidogen in its ground electronic and vibrational state ((X) over tilde (3)Sigma(-)) was carried out in the THz range (up to 225 cm(-1)) with the AILES beamline of the SOLEIL synchrotron and subsequently with the PhLAM spectrometer (around 942 GHz). The observed fine and hyperfine structures were analysed, yielding an accurate set of rotational, fine, and hyperfine parameters. Results. The reported frequencies and molecular constants are suitable for radioastronomical searches of this key species and for N-14/N-15 isotopic ratio astronomical determination.
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Barroca, T., Balaa, K., Leveque-Fort, S., & Fort, E. (2012). Full-field near-field optical microscope for cell imaging. PHYSICAL REVIEW LETTERS, 108(21), 218101.
Résumé: We report a new full-field fluorescence microscopy method for imaging live cell membranes based on supercritical near-field emission. This technique consists of extracting the self-interference between undercritical and supercritical light by simple image subtraction. In the objective back focal plane, this is equivalent to adding a virtual mask blocking the subcritical emission. We show that this virtual mask is radically different from a real physical mask, enabling a 100 nm axial confinement and enhancing the image sensitivity without damaging the lateral resolution. This technique is easy to implement and simultaneously provides images of the inner parts of the cell and its membrane with standard-illumination light.
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Bergeron, H., Curado, E. M. F., Gazeau, J. P., & Rodrigues, L. M. C. S. (2012). Generating functions for generalized binomial distributions. JOURNAL OF MATHEMATICAL PHYSICS, 53(10), 103304.
Résumé: In a recent article generalization of the binomial distribution associated with a sequence of positive numbers was examined. The analysis of the nonnegativeness of the formal probability distributions was a key point to allow to give them a statistical interpretation in terms of probabilities. In this article we present an approach based on generating functions that solves the previous difficulties. Our main theorem makes explicit the conditions under which those formal probability distributions are always non-negative. Therefore, the constraints of non-negativeness are automatically fulfilled giving a complete characterization in terms of generating functions. A large number of analytical examples becomes available. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4757601]
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Bergeron, H., Siegl, P., & Youssef, A. (2012). New SUSYQM coherent states for Poschl-Teller potentials: a detailed mathematical analysis. JOURNAL OF PHYSICS A-MATHEMATICAL AND THEORETICAL, 45(24).
Résumé: In a recent short note (Bergeron et al 2010 Europhys. Lett. 92 60003), we have presented the good properties of a new family of semi-classical states for Poschl-Teller potentials. These states are built from a supersymmetric quantum mechanics (SUSYQM) approach and the parameters of these 'coherent' states are points in the classical phase space. In this paper, we develop all the mathematical aspects that have been left out of the previous paper (proof of the resolution of unity, detailed calculations of the quantized version of classical observables and mathematical study of the resulting operators: problems of domains, self-adjointness or self-adjoint extensions). Some additional questions such as asymptotic behavior are also studied. Moreover, the framework is extended to a larger class of Poschl-Teller potentials. This article is part of a special issue of Journal of Physics A: Mathematical and Theoretical devoted to 'Coherent states: mathematical and physical aspects'.
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Billaud, P., Geleoc, M., Picard, Y. J., Veyrinas, K., Hergott, J. F., Poullain, S. M., Breger, P., Ruchon, T., Roulliay, M., Delmotte, F., Lepetit, F., Huetz, A., Carre, B., & Dowek, D. (2012). Molecular frame photoemission in dissociative ionization of H-2 and D-2 induced by high harmonic generation femtosecond XUV pulses. JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 45(19), 194013.
Résumé: We report the first results of molecular frame photoelectron emission for dissociative photoionization (DPI) of H-2 and D-2 molecules induced by a spectrally filtered single high harmonic of a few femtosecond duration, using coincident electron-ion velocity vector correlation techniques. For the studied photon energies around 32 eV, where the resonant excitation of the Q(1) and Q(2) doubly excited states occurs, autoionization and nuclear dynamics are coupled on a few femtosecond timescale, giving rise to quantum interferences. Molecular frame photoelectron angular distributions (MFPADs), traced as a function of the kinetic energy release of the atomic fragments, provide the most sensitive observables for such complex dynamics. These results compare well with recent spectrally resolved experiments using synchrotron radiation which are also reported. As a novel XUV light source running at multi-kHz repetition rate and synchronized with laser pulses, high-order harmonic generation (HHG) opens new possibilities for extending these investigations to time-resolved studies at the femtosecond scale.
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Blancard, C., Cosse, P., Faussurier, G., Bizau, J. - M., Cubaynes, D., El Hassan, N., Guilbaud, S., Al Shorman, M. M., Robert, E., Liu, X. - J., Nicolas, C., & Miron, C. (2012). L-shell photoionization of Ar+ to Ar3+ ions. PHYSICAL REVIEW A, 85(4), 043408.
Résumé: Absolute photoionization cross sections of Ar+, Ar2+, and Ar3+ ions have been measured in the 250-280 eV photon energy range. These results are compared to theoretical cross sections extracted from two new calculations we performed. They reproduce well the general behavior of the experimental spectra and the magnitude of the direct photoionization cross sections. However, the oscillator strength of the resonant structure in the spectra, dominated by 2p -> 3d transitions, is overestimated up to 80% by our calculations.
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Borges, C. V. S., Khoury, A. Z., Walborn, S., Ribeiro, P. H. S., Milman, P., & Keller, A. (2012). Bell inequalities with continuous angular variables. Phys. Rev. A., 86(5), 052107.
Résumé: We consider bipartite quantum systems characterized by a continuous angular variable., representing, for instance, the position of a particle on a circle or in a periodic lattice. For this type of system, we show how to violate inequalities similar to Clauser-Horne-Shimony-Holt (CHSH) ones, originally derived for bipartite spin-1/2-like systems. Such inequalities involve correlated measurement of continuous angular functions and are equivalent to the continuous superposition of CHSH inequalities acting on bidimensional subspaces of the infinite dimensional Hilbert space. As an example, we discuss in detail one application of our results, and we derive inequalities based on orientation correlation measurements. The introduced Bell-type inequalities open the perspective of new and simpler experiments to test the assumptions of locality, realism, or freedom of choice in a variety of quantum systems described by continuous variables. We discuss in detail a possible implementation using the orbital angular momentum of photons.
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Borisov, A. G., Echenique, P. M., & Kazansky, A. K. (2012). Attostreaking with metallic nano-objects. New J. Phys., 14, 023036.
Résumé: The application of atto-second streaking spectroscopy (ASS) to direct time-domain studies of the plasmonic excitations in metallic nano-objects is addressed theoretically. The streaking spectrograms for a rectangular gold nano-antenna and spherical gold clusters are obtained within strong field approximation using classical electron trajectory calculations. The results reported here for spherical clusters are also representative of spherical nano-shells. This study demonstrates that ASS allows for detailed characterization of plasmonic modes, including near-field enhancement, frequency and decay rate. The role of the inhomogeneity of the induced electric fields is also demonstrated.
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Boudrioua, O., Yang, H., Sonnet, P., Stauffer, L., Mayne, A. J., Comtet, G., Dujardin, G., Kuk, Y., Nagarajan, S., Gourdon, A., & Duverger, E. (2012). Large organic molecule chemisorption on the SiC(0001) surface. Phys. Rev. B, 85(3), 035423.
Résumé: We present a density-functional theory (DFT) study combined with scanning tunneling microscopy (STM) experiments of the chemisorption of the N,N'-bis(1-hexylheptyl) perylene-3,4:9,10-bis(dicarboximide) molecule, noted here as DHH-PTCDI, on the SiC(0001)-3 x 3 surface. Five possible adsorption configurations have been investigated in which molecular adsorption occurs on two adjacent Si adatoms via different pairs of atoms of the molecule. We have calculated the energies, structures, density of states, local density of states, and a calculated STM image and show that chemisorption via two oxygen atoms located on the same side of the molecule on two adjacent Si adatoms is the most favorable, in agreement with the experimental STM images. A comparison between the PTCDI and the adsorption of another large organic molecule (phthalocyanine) on the SiC(0001) surface completes this work.
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Bulard, E., Fontaine-Aupart, M. - P., Dubost, H., Zheng, W., Bellon-Fontaine, M. - N., Herry, J. - M., & Bourguignon, B. (2012). Competition of Bovine Serum Albumin Adsorption and Bacterial Adhesion onto Surface-Grafted ODT: In Situ Study by Vibrational SFG and Fluorescence Confocal Microscopy. Langmuir, 28(49), 17001–17010.
Résumé: The interaction of hydrophilic and hydrophobic ovococcoid bacteria and bovine serum albumin (BSA) proteins with a well ordered surface of octadecanethiol (ODT) self assembled monolayer (SAM) has been studied in different situations where proteins were either preadsorbed on ODT or adsorbed simultaneously with bacterial adhesion as in life conditions. The two situations lead to very different antimicrobial behavior. Bacterial adhesion on preadsorbed BSA is very limited, while the simultaneous exposure of ODT SAM to proteins and bacteria lead to a markedly weaker antimicrobial effect. The combination of sum frequency generation spectroscopy and fluorescence confocal microscopy experiments allow one to draw conclusions on the factors that govern the ODT SAM or BSA film interaction with bacteria at the molecular level. On the hydrophobic ODT surface, interaction with hydrophobic or hydrophilic biomolecules results in opposite effects on the SAM, namely, a flattening or a raise of the terminal methyl groups of ODT. On an amphiphilic BSA layer, the bacterial adhesion strength is weakened by the negative charges carried by both BSA and bacteria. Surprisingly, preadsorbed BSA that cover part of the bacteria cell walls increase the adhesion strength to the BSA film and reduce hydrophobic interactions with the ODT SAM. Finally, bacterial adhesion on a BSA film is shown to modify the BSA proteins in some way that change their interaction with the ODT SAM. The antimicrobial effect is much stronger in the case of a preadsorbed BSA layer than when BSA and bacteria are in competition to colonize the ODT SAM surface.
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Bulard, E., Fontaine-Aupart, M. - P., Dubost, H., Zheng, W., Herry, J. - M., Bellon-Fontaine, M. - N., Briandet, R., & Bourguignon, B. (2012). The Effect of Bacterial Adhesion on Grafted Chains Revealed by the Non-Invasive Sum Frequency Generation Spectroscopy. Spectrosc.-Int. J., 27(5-6), 571–579.
Résumé: In biomedical and food industry, surface colonization by bacteria is harmful: it leads to biofilm formation, a microbial consortia more resistant to antibiotics than planktonic bacteria. In order to design materials able to limit the biofilm formation, the effect of bacteria on materials has to be well characterized. In this work, a well-defined surface composed of a self-assembled monolayer (SAM) of octadecanethiol (ODT) onto a gold surface is probed in situ. The SAM conformation is obtained using the femtosecond vibrational sum frequency generation (SFG) spectroscopy. This technique provides selectively the molecular vibrational signature of the interface. The behaviour of the ODT SAM is studied in different environments: in air, in water, and upon exposure to hydrophilic or hydrophobic Lactococcus lactis bacteria. Modelling the experimental SFG spectra reveals a measurable change of the SAM conformation which depends on the environment, especially on the hydrophilic-hydrophobic character.
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Calvo, F., & Parneix, P. (2012). Amplification of Anharmonicities in Multiphoton Vibrational Action Spectra. CHEMPHYSCHEM, 13(1), 212–220.
Résumé: The influence of one or several infrared laser pulses on the stability of bare and argon-tagged sodium chloride clusters is investigated theoretically by a combination of computational methods involving explicit molecular dynamics and properly calibrated unimolecular rate theories. The fragmentation spectra obtained by varying the laser frequency in the far-IR range is compared to the linear absorption spectrum resulting from the dipole moment autocorrelation function. Under appropriate laser field parameters, the action spectra are found to resemble the absorption spectra quite accurately in terms of positions, line widths, and even relative intensities. However, the action spectra exhibit residual and systematic redshifts of a few percent, which are partly due to the finite spectral bandwidth but are amplified by the progressive heating by the laser. A quantitative analysis suggests that these anharmonicity effects should generally arise upon multiple photon absorption.
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Calvo, F., & Parneix, P. (2012). Multiscale modeling of vibrational predissociation spectra under a chirped laser pulse. EUROPEAN PHYSICAL JOURNAL D, 66(6), 165.
Résumé: The vibrational predissociation spectrum of the argon-tagged ionic cluster (NaCl)(32) due to exposure to a chirped infrared laser was theoretically calculated in a time multiscale framework. The response to the laser field is modeled explicitly by molecular dynamics simulations, and statistical rate theories are used to evaluate the long-time dissociation probability. Due to anharmonicities and multiphoton processes, the predissociation spectrum shows some small but systematic red shift in the main absorption line. Negative chirping toward lower frequencies further enhances this effect, and also alters the band intensity and the band width. Positive chirping attenuates the dissociation efficiency.
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Calvo, F., Nguyen-Thi Van-Oanh, Parneix, P., & Falvo, C. (2012). Vibrational spectra of polyatomic molecules assisted by quantum thermal baths. PHYSICAL CHEMISTRY CHEMICAL PHYSICS, 14(30), 10503–10506.
Résumé: We assess the performance of colored-noise thermostats to generate quantum mechanical initial conditions for molecular dynamics simulations, in the context of infrared spectra of large polyatomic molecules. Comparison with centroid molecular dynamics simulations taken as reference shows that the method is accurate in predicting line shifts and band widths in the ionic cluster (NaCl) 32 and in the naphthalene molecule. As illustrated on much larger polycyclic aromatic hydrocarbons, the method also allows fundamental spectra to be evaluated in the limit of T = 0, taking into account anharmonicities and vibrational delocalization.
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Carpentier, Y., Feraud, G., Dartois, E., Brunetto, R., Charon, E., Cao, A. T., d'Hendecourt, L., Brechignac, P., Rouzaud, J. N., & Pino, T. (2012). Nanostructuration of carbonaceous dust as seen through the positions of the 6.2 and 7.7 μm AIBs. ASTRONOMY & ASTROPHYSICS, 548, A40.
Résumé: Context. Carbonaceous cosmic dust is observed through infrared spectroscopy either in absorption or in emission. The details of the spectral features are believed to shed some light on its structure and finally enable the study of its life cycle. Aims. The goal is to combine several analytical tools in order to decipher the intimate nanostructure of some soot samples. Such materials provide interesting laboratory analogues of cosmic dust. In particular, spectroscopic and structural characteristics that help to describe the polyaromatic units embedded into the soot, including their size, morphology, and organisation are explored. Methods. Laboratory analogues of the carbonaceous interstellar and circumstellar dust were produced in fuel-rich low-pressure, premixed and flat flames. The soot particles were investigated by infrared absorption spectroscopy in the 2-15 μm spectral region. Raman spectroscopic measurements and high-resolution transmission electron microscopy were performed, which offered complementary information to better delineate the intimate structure of the analogues. Results. These laboratory analogues appeared to be mainly composed of sp(2) carbon, with a low sp(3) carbon content. A cross relation between the positions of the aromatic C=C bands at about 6.2 micron and the band at about 8 micron is shown to trace differences in shapes and structures of the polyaromatic units in the soot. Such effects are due to the defects of the polyaromatic structures in the form of non-hexagonal rings and/or aliphatic bridges. The role of these defects is thus observed through the 6.2 and 7.7 μm aromatic infrared band positions, and a distinction between carriers composed of curved aromatic sheets and more planar ones can be inferred. Based on these nanostructural differences, a scenario of nanograin growth and evolution is proposed.
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Cassimi, A., Ikeda, T., Maunoury, L., Zhou, C. L., Guillous, S., Mery, A., Lebius, H., Benyagoub, A., Grygiel, C., Khemliche, H., Roncin, P., Merabet, H., & Tanis, J. A. (2012). Dynamics of charge evolution in glass capillaries for 230-keV Xe23+ ions. Phys. Rev. A, 86(6), 062902.
Résumé: We have measured the transmission of 230-keV (10-keV/q) Xe23+ ions through insulating tapered glass capillaries of microscopic dimensions. The dynamics of charging and discharging processes have been investigated, evidencing an unexpected slow alignment of the beam along the capillary axis. Oscillations of the exiting beam position have been observed during the charging process associated to the formation of charge patches on the capillary inner walls. The emerging ions are guided with a characteristic guiding angle falling on a universal curve proposed for PET polymer nanocapillaries. This result, very similar to the channeling process, is somewhat surprising in view of the significant differences between the straight nanocapillary polymer foils and the tapered microscopic single glass capillary used here. The transmitted ions show no evidence of energy loss or charge changing except for the production of a small neutral fraction that was determined to be due to ions that had become neutralized to form atoms rather than due to photon emission. These results thus test and confirm the validity of transmission and guiding and provide insight into the dynamics of higher-energy ions than have been previously studied in this regard, allowing a determination of the maximum energy for which the guiding process might occur.
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Chaabouni, H., Bergeron, H., Baouche, S., Dulieu, F., Matar, E., Congiu, E., Gavilan, L., & Lemaire, J. L. (2012). Sticking coefficient of hydrogen and deuterium on silicates under interstellar conditions. ASTRONOMY & ASTROPHYSICS, 538, A128.
Résumé: Context. Sticking of H and D atoms on interstellar dust grains is the first step in molecular hydrogen formation, which is a key reaction in the interstellar medium. Isotopic properties of the sticking can have an incidence on the observed HD molecule. Aims. After studying the sticking coefficients of H-2 and D-2 molecules on amorphous silicate surfaces experimentally and theoretically, we extrapolate the results to the sticking coefficient of atoms and propose a formulae that gives the sticking coefficients of H and D on both silicates and icy dust grains. Methods. In our experiments, we used the King and Wells method for measuring the sticking coefficients of H-2 and D-2 molecules on a silicate surface held at 10 K. It consists of measuring with a QMS (quadrupole mass spectrometer) the signals of H-2 and D-2 molecules reflected by the surface during the exposure of the sample to the molecular beam at a temperature ranging from 20 K to 340 K. We tested the efficiency of a physical model, developed previously for sticking on water-ice surfaces. We applied this model to our experimental results for the sticking coefficients of H-2 and D-2 molecules on a silicate surface and estimated the sticking coefficient of atoms by a single measurement of atomic recombination and propose an extrapolation. Results. Sticking of H, D, HD, H-2, and D-2 on silicates grains behaves the same as on icy dust grains. The sticking decreases with the gas temperature, and is dependent on the mass of the impactor. The sticking coefficient for both surfaces and impactors can be modeled by an analytical formulae S (T) = S-0(1 + beta T/ T-0)/(1 + T/T-0)(beta), which describes both the experiments and the thermal distribution expected in an astrophysical context. The parameters S-0 and T-0 are summarized in a table. Conclusions. Previous estimates for the sticking coefficient of H atoms are close to the new estimation; however, we find that, when isotopic effects are taken into account, the sticking coefficient variations can be as much as a factor of 2 at T = 100 K.
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Cuisset, A., Pirali, O., & Sadovskii, D. A. (2012). Gyroscopic Destabilization of Molecular Rotation and Quantum Bifurcation Observed in the Structure of the nu(23) Fundamental of Dimethylsulfoxyde. PHYSICAL REVIEW LETTERS, 109(9), 094101.
Résumé: Following the first successful high-resolution study of the “perpendicular” band of dimethylsulfoxyde at 324 cm(-1), associated with the nu(23) bending vibration, we discovered a sequence of fourfold degenerate clusters of rotational levels at high angular momenta J > 40. This unusual system of localized states corresponds to classical rotations about a pair of “tilted” axes, which become stationary at high J, after the principal axis of inertia A loses stability and bifurcates for J approximate to 27.
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Daddi Oubekka, S., Briandet, R., Fontaine-Aupart, M. - P., & Steenkeste, K. (2012). Correlative time-resolved fluorescence microscopy to assess antibiotic diffusion-reaction in biofilms. Antimicrobial agents and chemotherapy, 56(6), 3349–58.
Résumé: The failure of antibiotics to inactivate in vivo pathogens organized in biofilms has been shown to trigger chronic infections. In addition to mechanisms involving specific genetic or physiological cell properties, antibiotic sorption and/or reaction with biofilm components may lessen the antibiotic bioavailability and consequently decrease their efficiency. To assess locally and accurately the antibiotic diffusion-reaction, we used for the first time a set of advanced fluorescence microscopic tools (fluorescence recovery after photobleaching, fluorescence correlation spectroscopy, and fluorescence lifetime imaging) that offer a spatiotemporal resolution not available with the commonly used time-lapse confocal imaging method. This set of techniques was used to characterize the dynamics of fluorescently labeled vancomycin in biofilms formed by two Staphylococcus aureus human isolates. We demonstrate that, at therapeutic concentrations of vancomycin, the biofilm matrix was not an obstacle to the diffusion-reaction of the antibiotic that can reach all cells through the biostructure.
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Dai, X., Richter, M., Li, H., Bristow, A. D., Falvo, C., Mukamel, S., & Cundiff, S. T. (2012). Two-Dimensional Double-Quantum Spectra Reveal Collective Resonances in an Atomic Vapor. PHYSICAL REVIEW LETTERS, 108(19), 193201.
Résumé: We report the observation of double-quantum coherence signals in a gas of potassium atoms at twice the frequency of the one-quantum coherences. Since a single atom does not have a state at the corresponding energy, this observation must be attributed to a collective resonance involving multiple atoms. These resonances are induced by weak interatomic dipole-dipole interactions, which means that the atoms cannot be treated in isolation, even at a low density of 10(12) cm(-3).
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Deniset-Besseau, A., Miannay, F. - A., Laplace-Builhe, C., Vielh, P., Lecart, S., Lwaleed, B. A., Eschwege, P., & Fontaine-Aupart, M. - P. (2012). A fluorescence-based assay for monitoring clinical drug resistance. JOURNAL OF CLINICAL PATHOLOGY, 65(11), 1003–1007.
Résumé: Background and aims Multidrug resistance (MDR) limits effectiveness in treating malignancy by modifying internalisation and/or externalisation of drugs through cancer cell membranes. In this study we describe an assay to monitor patients' responses to chemotherapy. Methods The assay is based on the fluorescent properties of doxorubicin alone as well as in combination with methotrexate, vinblastine, doxorubicin and cisplatin (MVAC). The slide-based cell imaging technique was first optimised using a panel of breast and urothelial cancer cell lines and then extended to fine needle breast aspiration biopsy and urine cytology. Results The drug fluorescence behaviour observed on smears of clinical specimens is identical to that obtained using fixed cultured cells. The fluorescence of sensitive cells to chemotherapy is mainly localised in the nucleus, whereas resistant cells show a weak fluorescence signal localised in the cytoplasm. The difference in terms of fluorescence intensity is also highlighted through fluorescence spectra. Conclusions The results suggest that the assay provides clinically valuable information in predicting responses to doxorubicin and/or MVAC therapy. Originally set up on a confocal microscope, the assay was also effective using a standard epifluorescence microscope; as such it is technically simple, reliable and inexpensive.
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Devauges, V., Marquer, C., Lecart, S., Cossec, J. - C., Potier, M. - C., Fort, E., Suhling, K., & Leveque-Fort, S. (2012). Homodimerization of Amyloid Precursor Protein at the Plasma Membrane: A homoFRET Study by Time-Resolved Fluorescence Anisotropy Imaging. PloS one, 7(9), e44434.
Résumé: Classical FRET (Forster Resonance Energy Transfer) using two fluorescent labels (one for the donor and another one for the acceptor) is not efficient for studying the homodimerization of a protein as only half of the homodimers formed can be identified by this technique. We thus resorted to homoFRET detected by time-resolved Fluorescence Anisotropy IMaging (tr-FAIM). To specifically image the plasma membrane of living cells, an original combination of tr-FAIM and Total Internal Reflection Fluorescence Lifetime Imaging Microscope (TIRFLIM) was implemented. The correcting factor accounting for the depolarization due to the high numerical aperture (NA) objective, mandatory for TIRF microscopy, was quantified on fluorescein solutions and on HEK293 cells expressing enhanced Green Fluorescence Protein (eGFP). Homodimerization of Amyloid Precursor Protein (APP), a key mechanism in the etiology of Alzheimer's disease, was measured on this original set-up. We showed, both in epifluorescence and under TIRF excitation, different energy transfer rates associated with the homodimerization of wild type APP-eGFP or of a mutated APP-eGFP, which forms constitutive dimers. This original set-up thus offers promising prospects for future studies of protein homodimerization in living cells in control and pathological conditions.
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Enriquez, H., Mayne, A. J., Kara, A., Vizzini, S., Roth, S., Lalmi, B., Seitsonen, A. P., Aufray, B., Greber, T., Belkhou, R., Dujardin, G., & Oughaddou, H. (2012). Adsorption of silicon on Au(110): An ordered two dimensional surface alloy. APPLIED PHYSICS LETTERS, 101(2), 021605.
Résumé: We report on experimental evidence for the formation of a two dimensional Si/Au(110) surface alloy. In this study, we have used a combination of scanning tunneling microscopy, low energy electron diffraction, Auger electron spectroscopy, and ab initio calculations based on density functional theory. A highly ordered and stable Si-Au surface alloy is observed subsequent to growth of a sub-monolayer of silicon on an Au(110) substrate kept above the eutectic temperature. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4735310]
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Enriquez, H., Vizzini, S., Kara, A., Lalmi, B., & Oughaddou, H. (2012). Silicene structures on silver surfaces. JOURNAL OF PHYSICS-CONDENSED MATTER, 24(31), 314211.
Résumé: In this paper we report on several structures of silicene, the analog of graphene for silicon, on the silver surfaces Ag(100), Ag(110) and Ag(111). Deposition of Si produces honeycomb structures on these surfaces. In particular, we present an extensive theoretical study of silicene on Ag(111) for which several recent experimental studies have been published. Different silicene structures were obtained only by varying the silicon coverage and/or its atomic arrangement. All the structures studied show that silicene is buckled, with a Si-Si nearest neighbor distance varying between 2.28 and 2.5 angstrom. Due to the buckling in the silicene sheet, the apparent (lateral) Si-Si distance can be as low as 1.89 angstrom. We also found that for a given coverage and symmetry, one may observe different scanning tunneling microscopy images corresponding to structures that differ by only a translation.
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Esteban, R., Borisov, A. G., Nordlander, P., & Aizpurua, J. (2012). Bridging quantum and classical plasmonics with a quantum-corrected model. Nat. Commun., 3, 825.
Résumé: Electromagnetic coupling between plasmonic resonances in metallic nanoparticles allows for engineering of the optical response and generation of strong localized near-fields. Classical electrodynamics fails to describe this coupling across sub-nanometer gaps, where quantum effects become important owing to non-local screening and the spill-out of electrons. However, full quantum simulations are not presently feasible for realistically sized systems. Here we present a novel approach, the quantum-corrected model (QCM), that incorporates quantum-mechanical effects within a classical electrodynamic framework. The QCM approach models the junction between adjacent nanoparticles by means of a local dielectric response that includes electron tunnelling and tunnelling resistivity at the gap and can be integrated within a classical electrodynamical description of large and complex structures. The QCM predicts optical properties in excellent agreement with fully quantum mechanical calculations for small interacting systems, opening a new venue for addressing quantum effects in realistic plasmonic systems.
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Falvo, C., Calvo, F., & Parneix, P. (2012). Probing the spin multiplicity of gas-phase polycyclic aromatic hydrocarbons through their infrared emission spectrum: A theoretical study. JOURNAL OF CHEMICAL PHYSICS, 137(6), 064303.
Résumé: The anharmonic infrared emission spectrum following an optical excitation has been calculated for a variety of polycyclic aromatic hydrocarbon molecules in their ground singlet electronic state or in their triplet state. The computational protocol relies on second-order perturbation theory and involves a quartic vibrational Hamiltonian, the vibrational quantum numbers being sampled according to a Monte Carlo procedure. In the case of neutral naphthalene, the IR spectrum obtained in the (ground) singlet state differs significantly from the spectrum in the triplet state, especially for out-of-plane CH bending modes. Although not as prominent, spectral differences in larger molecules are still observable.
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Falvo, C., Zhuang, W., Kim, Y. S., Axelsen, P. H., Hochstrasser, R. M., & Mukamel, S. (2012). Frequency Distribution of the Amide-I Vibration Sorted by Residues in Amyloid Fibrils Revealed by 2D-IR Measurements and Simulations. JOURNAL OF PHYSICAL CHEMISTRY B, 116(10), 3322–3330.
Résumé: The infrared optical response of amyloid fibrils A beta(1-40) is investigated. Simulations of two models corresponding to different protonation states are compared with experiment. The simulations reveal that vibrational frequency distributions inside the fibrils are dominated by side chain fluctuations. We further confirm earlier suggestions based on 2D-IR measurements that water molecules can be trapped inside the fibrils.
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Fan, C., Poumellec, B., Zeng, H., Desmarchelier, R., Bourguignon, B., Chen, G., & Lancry, M. (2012). Gold Nanoparticles Reshaped by Ultrafast Laser Irradiation Inside a Silica-Based Glass, Studied Through Optical Properties. J. Phys. Chem. C, 116(4), 2647–2655.
Résumé: Quasi-spherical or quasi-rod gold nanoparticles with an average diameter of 3.8 nm are randomly precipitated in a silica-based glass by a heat-treatment method. After ultrafast laser irradiation at 400 and 620 nm, optical absorption, birefringence, and dichroism measurements are performed to investigate the modification of gold nanoparticles shape. Theoretical simulations have been carried out to interpret the experimental results. We suggest that a small fraction of gold nanospheres are transformed mainly into nanodisks but also into nanorods oriented along the laser polarization for both fs laser wavelength. Absorption simulation suggests that they have an aspect ratio of 1.8 and 0.5, respectively, for fs laser irradiation at 400 nm. For 620 nm, the aspect ratio of the nanorods increases and the one of the nanodisks decreases. In such a way, we demonstrate that reshaping of gold nanoparticles, i.e. a property that was previously found for silver nanoparticles in multicomponent glass is also possible. By imaging the distribution of the birefringence according to the probe wavelength, we show that nanopartides are aligned into nanorods mainly out of irradiated volume and into nanopellets mainly in the irradiated volume.
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Gamache, R. R., Lamouroux, J., Laraia, A. L., Hartmann, J. - M., & Boulet, C. (2012). Semiclassical calculations of half-widths and line shifts for transitions in the 30012 <- 00001 and 30013 <- 00001 bands of CO2, I: Collisions with N-2. JOURNAL OF QUANTITATIVE SPECTROSCOPY & RADIATIVE TRANSFER, 113(11), 976–990.
Résumé: Calculations of the half-width, its temperature dependence, and the line shift are made for the rotational states J = 0-120 for two of the Fermi-tetrad bands (30012 <- 00001 and 30013 <- 00001) of CO2 perturbed by N-2. The calculations employ the semi-classical complex Robert-Bonamy method with no ad hoc scaling, J-dependent or otherwise, and an intermolecular potential (IP) comprised of an electrostatic part, an atom-atom part, and an isotropic London dispersion part. The averaging over the impact parameter b and relative speed v are explicitly carried out. Many interesting features about CO2 as the radiating molecule are elucidated. Effects of the trajectory model, the order of the expansion of the atom-atom component of the potential, and the inclusion of the imaginary terms are studied. It is shown that the results are very sensitive to the intermolecular potential. The final IP parameters give results that demonstrate excellent agreement with measurement for the three line shape parameters studied in this work. (C) 2012 Elsevier Ltd. All rights reserved.
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Garcia-Gil, S., Garcia, A., & Ordejon, P. (2012). Calculation of core level shifts within DFT using pseudopotentials and localized basis sets. EUROPEAN PHYSICAL JOURNAL B, 85(7), 239.
Résumé: The calculation of core level shifts can be done in the context of density functional theory (DFT) using different approaches and physical approximations to the photoemission process. The initial state and the Delta SCF approximations are the most commonly used ones. Here, we describe the details of their implementation in the context of DFT using pseudopotentials and localized atomic orbitals as a basis set, and in particular as applied to the Siesta code. We give a full account of the technicalities involved in these calculations, including the details of the ionic pseudopotential generation, basis sets, charge states and reference potential. We test the method by computing the core level shifts of the Si 2p level for a series of molecules and the p(2x2) asymmetric- dimer reconstruction of the Si(001) surface.
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Gauyacq, J. - P., Lorente, N., & Dutilh Novaes, F. (2012). Excitation of local magnetic moments by tunneling electrons. Prog. Surf. Sci., 87(5-8), 63–107.
Résumé: The advent of milli-kelvin scanning tunneling microscopes (STM) with inbuilt magnetic fields has opened access to the study of magnetic phenomena with atomic resolution at surfaces. In the case of single atoms adsorbed on a surface, the existence of different magnetic energy levels localized on the adsorbate is due to the breaking of the rotational invariance of the adsorbate spin by the interaction with its environment, leading to energy terms in the meV range. These structures were revealed by STM experiments in IBM Almaden in the early 2000s for atomic adsorbates on CuN surfaces. The experiments consisted in the study of the changes in conductance caused by inelastic tunneling of electrons (IETS, inelastic electron tunneling spectroscopy). Manganese and Iron adatoms were shown to have different magnetic anisotropies induced by the substrate. More experiments by other groups followed up, showing that magnetic excitations could be detected in a variety of systems: e.g. complex organic molecules showed that their magnetic anisotropy was dependent on the molecular environment, piles of magnetic molecules showed that they interact via intermolecular exchange interaction, spin waves were excited on ferromagnetic surfaces and in Mn chains, and magnetic impurities have been analyzed on semiconductors. These experiments brought up some intriguing questions: the efficiency of magnetic excitations was very high, the excitations could or could not involve spin flip of the exciting electron and singular-like behavior was sometimes found at the excitation thresholds. These facts called for extended theoretical analysis: perturbation theories, sudden-approximation approaches and a strong coupling scheme successfully explained most of the magnetic inelastic processes. In addition, many-body approaches were also used to decipher the interplay between inelastic processes and the Kondo effect. Spin torque transfer has been shown to be effective in changing spin orientations of an adsorbate in theoretical works, and soon after it was shown experimentally. More recently, the previously mentioned strong coupling approach was extended to treat the excitation of spin waves in atomic chains and the ubiquitous role of electron-hole pair creation in de-exciting spins on surfaces has been analyzed. This review article expounds these works, presenting the theoretical approach by the authors while trying to thoroughly review parallel theoretical and experimental works. (C) 2012 Elsevier Ltd. All rights reserved.
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Gauyacq, J. P., & Lorente, N. (2012). Lifetime of magnetic excitations in supported ferromagnetic and antiferromagnetic spin-1/2 Heisenberg chains. PHYSICAL REVIEW B, 85(11), 115420.
Résumé: The lifetime of magnetic excitations in finite 1D-supported Heisenberg chains of magnetic atoms is studied theoretically for a model system formed of S = 1/2 spins. Both ferromagnetic and antiferromagnetic cases are considered as well as open chains and rings of atoms. Different chain lengths are considered allowing extrapolation to infinite chains. All the excited magnetic states in the finite chains and rings are studied, not only the spin-wave mode. The magnetic excitations decay by electron-hole pair creation in the substrate. As the main result, for all the systems considered, the decay rate appears to vary approximately proportionally to the excitation energy of the state, with a proportionality constant independent of the strength of the Heisenberg exchange term. In certain finite systems, a stable state is evidenced at low energy, associated with a special spin coupling structure.
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Grammenos, A., Fillet, M., Collodoro, M., Lecart, S., Quoilin, C., Fontaine-Aupart, M. - P., & Hoebeke, M. (2012). An ESR, Mass Spectrometry and Fluorescence Microscopy Approach to Study the Stearic Acid Derivatives Anchoring in Cells. APPLIED MAGNETIC RESONANCE, 43(3), 311–320.
Résumé: Lateral phase separations in biological membranes are of great interest, making electron spin resonance (ESR) spectroscopy combined with spin labeling a nondestructive and sensitive technique for the study of lipid rafts. It is currently accepted that the spin probe is localized on the plasma membrane. However, no study confirms this hypothesis. Herein, we report, for the first time, an accurate multispectral method for the quantification of the lipid spin label presence in every subcellular fraction. Cells were incubated with the 5-DOXYL stearic acid derivative and then subfractionated. Results of our multimodal spectroscopy approach ubiquitously demonstrate that the ESR spin label presence only sets in the plasma membranes.
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Hartmann, J. - M., & Boulet, C. (2012). Quantum and classical approaches for rotational relaxation and nonresonant laser alignment of linear molecules: A comparison for CO2 gas in the nonadiabatic regime. JOURNAL OF CHEMICAL PHYSICS, 136(18), 184302.
Résumé: A quantum approach and classical molecular dynamics simulations (CMDS) are proposed for the modeling of rotational relaxation and of the nonadiabatic alignment of gaseous linear molecules by a nonresonant laser field under dissipative conditions. They are applied to pure CO2 and compared by looking at state-to-state collisional rates and at the value of < cos(2)[theta(z)(t)]> induced by a 100 fs laser pulse linearly polarized along (z) over right arrow. The main results are: (i) When properly requantized, the classical model leads to very satisfactory predictions of the permanent and transient alignments under non-dissipative conditions. (ii) The CMDS calculations of collisional-broadening coefficients and rotational state-to-state rates are in very good agreement with those of a quantum model based on the energy corrected sudden (ECS) approximation. (iii) Both approaches show a strong propensity of collisions, while they change the rotational energy (i. e., J), to conserve the angular momentum orientation (i. e., M/J). (iv) Under dissipative conditions, CMDS and quantum-ECS calculations lead to very consistent decays with time of the “permanent” and transient components of the laser-induced alignment. This result, expected from (i) and (ii), is obtained only if a properly J- and M-dependent ECS model is used. Indeed, rotational state-to-state rates and the decay of the “permanent” alignment demonstrate, for pure CO2, the limits of a M-independent collisional model proposed previously. Furthermore, computations show that collisions induce a decay of the “permanent” alignment about twice slower than that of the transient revivals amplitudes, a direct consequence of (iii). (v) The analysis of the effects of reorienting and dephasing elastic collisions shows that the latter have a very small influence but that the former play a non-negligible role in the alignment dynamics. (vi) Rotation-translation collisionally induced transfers have also been studied, demonstrating that they only slightly change the alignment dissipation for the considered laser energy conditions. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4705264]
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Henchy, C., Murray, C., Crepin, C., & McCaffrey, J. G. (2012). A DFT study of reversed isotope shifts in H/D substitution of free-base porphyrin and related free-base tetrapyrroles. Can. J. Chem.-Rev. Can. Chim., 90(12), 1078–1091.
Résumé: DFT/B3LYP calculations are used to analyse the occurrence of reverse isotope shift ratios (ISR) in H/D substitution of the free-base tetrapyrroles, in situations where the frequency ratio v(H)/v(D) is less than 1. The reverse ISR effect is found to be most evident in the out-of-plane bending modes (b(2g) and b(3u), symmetry) involving some N-H motion for the four molecules studied, viz., porphine (H2P), tetraaza-porphine (H(2)TAP), tetrabenzo-porphine (H2TBP), and phthalocyanine (H2Pc). It was analysed by following the evolution of the normal mode frequencies with incremental variation of the H atom masses from 1 to 2 amu. This method allows direct, unambiguous mode correlations to be established between the light and the heavy isotopologues. When the NH(D) motion is predominant, the H to D frequency evolution decreases in a continuous manner for a particular normal mode. In the case of two modes of the same symmetry and whose frequencies are similar, their frequency evolutions could cross, depending on the extent of NH(D) motion involved in them. The evolution diagrams may show avoided crossings of various extents, which thereby reflects the degree of the NH(D) motion in the modes. The reverse ISR effect is directly correlated to these avoided crossings. Because the isotope shifts are quite small (<10 cm(-1)) and occur in the congested 1500-500 cm(-1) spectral region, high-resolution methods yielding narrow line transitions are required for experimental analysis. The matrix isolation technique is particularly well suited for this work and is proposed for use in a search for this effect.
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Herberth, D., Baum, O., Pirali, O., Roy, P., Thorwirth, S., Yamada, K. M. T., Schlemmer, S., & Giesen, T. F. (2012). Far infrared Fourier-transform spectroscopy of mono-deuterated hydrogen peroxide HOOD. JOURNAL OF QUANTITATIVE SPECTROSCOPY & RADIATIVE TRANSFER, 113(11), 1127–1133.
Résumé: We present the gas phase spectrum of singly deuterated hydrogen peroxide, HOOD, in its vibrational ground state, recorded by the high resolution Fourier-transform interferometer located at the AILES synchrotron beamline connected to SOLEIL More than 1000 transitions in the range from 20 to 143 cm(-1) were assigned, leading to a set of preliminary rotational and centrifugal distortion constants determined by least squares fit analysis. All transitions are split by the tunneling motion of a hindered internal rotation. The splitting has been determined to be 5.786(13)cm(-1) in the torsional ground state and it shows a dependence on the rotational quantum number K-a. Some perturbations were not treated yet, but the present analysis permits to obtain a preliminary set of parameters. (C) 2012 Elsevier Ltd. All rights reserved.
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Houzet, J., Gateau, J., Hertz, E., Billard, F., Lavorel, B., Hartmann, J. - M., Boulet, C., & Faucher, O. (2012). Probing ultrafast thermalization with field-free molecular alignment. PHYSICAL REVIEW A, 86(3), 033419.
Résumé: The rotation-translation thermalization of CO2 gas is investigated 500 ps after its preheating by a nonresonant short and intense laser pulse. The temperature of thermalization is optically determined with two additional short laser pulses enabling a field-free molecular alignment process and its probing, respectively. The measurements are performed for various intensities of the preheat pulse, leading to the observation of different temperatures which are in very good agreement with classical molecular dynamics simulations. The results can be regarded as a step towards real-time tracking of ultrafast relaxation pathways in molecular motion.
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Huet, T. R., Aviles Moreno, J. - R., Pirali, O., Tudorie, M., Partal Urena, F., & Lopez Gonzalez, J. - J. (2012). Terpenes in the gas phase: The Far-IR spectrum of perillaldehyde. JOURNAL OF QUANTITATIVE SPECTROSCOPY & RADIATIVE TRANSFER, 113(11), 1261–1265.
Résumé: The far infrared spectrum of S-(-)-perillaldehyde, a monoterpene containing an aldehyde functional group, has been recorded in the gas phase using FTIR spectroscopy. The vibration signature of the three most populated rotamers has been observed and identified in the 30-650 cm(-1) range. The vibration assignment was based on the scaled B3LYP/cc-pVDZ harmonic force field of Partal Urena et al., 2008 [10]. Anharmonic contributions calculated at the HF/6-31+G* level were found negligible. (C) 2011 Elsevier Ltd. All rights reserved.
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Ideguchi, T., Bernhardt, B., Guelachvili, G., Haensch, T. W., & Picque, N. (2012). Raman-induced Kerr-effect dual-comb spectroscopy. OPTICS LETTERS, 37(21), 4498–4500.
Résumé: We report on the first (to our knowledge) demonstration of nonlinear dual-frequency-comb spectroscopy. In multi-heterodyne femtosecond Raman-induced Kerr-effect spectroscopy, the Raman gain resulting from the coherent excitation of molecular vibrations by a spectrally narrow pump is imprinted onto the femtosecond laser frequency comb probe spectrum. The birefringence signal induced by the nonlinear interaction of these beams and the sample is heterodyned against a frequency comb local oscillator with a repetition frequency slightly different from that of the comb probe. Such time-domain interference provides multiplex access to the phase and amplitude Raman spectra over a broad spectral bandwidth within a short measurement time. (C) 2012 Optical Society of America
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Ideguchi, T., Poisson, A., Guelachvili, G., Haensch, T. W., & Picque, N. (2012). Adaptive dual-comb spectroscopy in the green region. OPTICS LETTERS, 37(23), 4847–4849.
Résumé: Dual-comb spectroscopy is extended to the visible spectral range with two short-pulse frequency-doubled free-running ytterbium-doped fiber lasers. When the spectrum is shifted to other domains by nonlinear frequency conversion, tracking the relative fluctuations of the femtosecond oscillators at their fundamental wavelength automatically produces the correction signal needed for the recording of distortion-free spectra. The dense rovibronic spectrum of iodine around 19; 240 cm(-1) is recorded within 12 ms at Doppler-limited resolution. (C) 2012 Optical Society of America
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Kaiser, F., Coudreau, T., Milman, P., Ostrowsky, D. B., & Tanzilli, S. (2012). Entanglement-Enabled Delayed-Choice Experiment. Science, 338(6107), 637–640.
Résumé: Wave-particle complementarity is one of the most intriguing features of quantum physics. To emphasize this measurement apparatus–dependent nature, experiments have been performed in which the output beam splitter of a Mach-Zehnder interferometer is inserted or removed after a photon has already entered the device. A recent extension suggested using a quantum beam splitter at the interferometer’s output; we achieve this using pairs of polarization-entangled photons. One photon is tested in the interferometer and is detected, whereas the other allows us to determine whether wave, particle, or intermediate behaviors have been observed. Furthermore, this experiment allows us to continuously morph the tested photon’s behavior from wavelike to particle-like, which illustrates the inadequacy of a naive wave or particle description of light.
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Kara, A., Enriquez, H., Seitsonen, A. P., Voon, L. C. L. Y., Vizzini, S., Aufray, B., & Oughaddou, H. (2012). A review on silicene-New candidate for electronics (vol 67, pg 1, 2012). SURFACE SCIENCE REPORTS, 67(5), 1–18.
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Korytar, R., Lorente, N., & Gauyacq, J. - P. (2012). Many-body effects in magnetic inelastic electron tunneling spectroscopy. Phys. Rev. B, 85(12), 125434.
Résumé: Magnetic inelastic electron tunneling spectroscopy (IETS) shows sharp increases in conductance when a new conductance channel associated with a change in magnetic structure is open. Typically, the magnetic moment carried by an adsorbate can be changed by collision with a tunneling electron; in this process the spin of the electron can flip or not. A previous one-electron theory [Phys. Rev. Lett. 103, 176601 (2009)] successfully explained both the conductance thresholds and the magnitude of the conductance variation. The elastic spin flip of conduction electrons by a magnetic impurity leads to the well-known Kondo effect. In the present work, we compare the theoretical predictions for inelastic magnetic tunneling obtained with a one-electron approach and with a many-body theory including Kondo-like phenomena. We apply our theories to a singlet-triplet transition model system that contains most of the characteristics revealed in magnetic IETS. We use two self-consistent treatments (noncrossing approximation and self-consistent ladder approximation). We show that, although the one-electron limit is properly recovered, new intrinsic many-body features appear. In particular, sharp peaks appear close to the inelastic thresholds; these are not localized exactly at thresholds and could influence the determination of magnetic structures from IETS experiments. Analysis of the evolution with temperature reveals that these many-body features involve an energy scale different from that of the usual Kondo peaks. Indeed, the many-body features perdure at temperatures much larger than the one given by the Kondo energy scale of the system.
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Koval, N. E., Sanchez-Portal, D., Borisov, A. G., & Diez Muino, R. (2012). Dynamic screening of a localized hole during photoemission from a metal cluster. Nanoscale Res. Lett., 7(1), 1–9.
Résumé: Recent advances in attosecond spectroscopy techniques have fueled the interest in the theoretical description of electronic processes taking place in the subfemtosecond time scale. Here we study the coupled dynamic screening of a localized hole and a photoelectron emitted from a metal cluster using a semi-classical model. Electron density dynamics in the cluster is calculated with time-dependent density functional theory, and the motion of the photoemitted electron is described classically. We show that the dynamic screening of the hole by the cluster electrons affects the motion of the photoemitted electron. At the very beginning of its trajectory, the photoemitted electron interacts with the cluster electrons that pile up to screen the hole. Within our model, this gives rise to a significant reduction of the energy lost by the photoelectron. Thus, this is a velocity-dependent effect that should be accounted for when calculating the average losses suffered by photoemitted electrons in metals.
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Labidi, H., Kantorovich, L., & Riedel, D. (2012). Atomic-scale control of hydrogen bonding on a bare Si(100)-2x1 surface. PHYSICAL REVIEW B, 86(16), 165441.
Résumé: The control of the dissociative adsorption of individual hydrogen molecules is performed on the silicon surface at the atomic scale. It is achieved using the tip of a low-temperature (9 K) scanning tunneling microscope (STM) exposed to 10(-6) torr of H-2 and by probing the bare Si(100)-2 x 1 surface at a positive bias. This effect is very localized and is induced by the tunnel electrons. The statistical study of this process reveals an activation energy threshold matching the creation of H-2(-) at the surface of the STM tip. Our results are supported by ab inito density functional calculations of a hydrogenated silicon dimer.
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Lalmi, B., Khemliche, H., Momeni, A., Soulisse, P., & Roncin, P. (2012). High resolution imaging of superficial mosaicity in single crystals using grazing incidence fast atom diffraction. J. Phys. Condens. Matter., 24(44), 442002.
Résumé: A new table top technique is used to simultaneously analyze the local morphology of crystalline surfaces as well as the misalignment of large scale domains at the topmost surface layer. The approach is based on fast atom diffraction at grazing incidence (GIFAD); the diffraction pattern yields the structural characteristics and the topology of the surface electronic density with atomic resolution. If superficial mosaicity is present, diffraction patterns arising from each mosaic domain can be distinguished, providing high sensitivity to the properties of each of the domains. Taking NaCl(001) as an example, we observe a discrete tilt angle distribution of the mosaic domains following an arithmetic progression with a 0.025 degrees +/- 0.005 degrees difference; a twist mosaic angle of 0.09 degrees +/- 0.01 degrees is also observed.
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Lamouroux, J., Gamache, R. R., Laraia, A. L., Hartmann, J. - M., & Boulet, C. (2012). Semiclassical calculations of half-widths and line shifts for transitions in the 30012 <- 00001 and 30013 <- 00001 bands of CO2 II: Collisions with O-2 and air. JOURNAL OF QUANTITATIVE SPECTROSCOPY & RADIATIVE TRANSFER, 113(11), 991–1003.
Résumé: The complex Robert-Bonamy (CRB) formalism was used to calculate the half-width, its temperature dependence, and the line shift for CO2 for transitions in the 30012 <- 00001 and 30013 <- 00001 bands with O-2 as the perturbing gas. The calculations were done for rotational quantum numbers from J=0 to J=120 with no ad hoc scaling of the line shape equations. The intermolecular potential parameters are adjusted on accurate experimental measurements of the half-widths, its temperature dependence, and the pressure-induced line shifts so that a single intermolecular potential reproduces all three parameters. Using the results of this work and previous results for N-2-broadening, air-broadening line shape parameters were also determined. The comparison of the CRB calculations with the experimental data available in the literature for the three line shape coefficients demonstrates the quality of the present calculations for the both bands under study. (C) 2012 Elsevier Ltd. All rights reserved.
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Lancry, M., Poumellec, B., Desmarchelier, R., & Bourguignon, B. (2012). Oriented creation of anisotropic defects by IR femtosecond laser scanning in silica. Opt. Mater. Express, 2(12), 1809–1821.
Résumé: Irradiation of non-luminescent silica with polarized IR femtosecond laser light produced a significant amount of luminescent defects. We have investigated the properties of luminescence produced by the defects using UV-VUV excitation experiment depending on the relative orientation of the laser polarization and its scanning direction. Silicon Oxygen Deficient Center (SiODC) is identified. SiODC related luminescence is much stronger when the excitation polarization is parallel to the sample scanning direction and moved at low velocity, regardless of the writing polarization direction. This indicates that the creation of this anisotropic defect is oriented by the movement of the femtosecond laser beam. (C)2012 Optical Society of America
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Le Sech, C., Kobayashi, K., Usami, N., Furusawa, Y., Porcel, E., & Lacombe, S. (2012). Comment on “Enhanced relative biological effectiveness of proton radiotherapy in tumor cells with internalized gold nanoparticles” [Appl. Phys. Lett. 98, 193702 (2011)]. APPLIED PHYSICS LETTERS, 100(2), 026101.
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Le Sech, C., Kobayashi, K., Usami, N., Furusawa, Y., Porcel, E., & Lacombe, S. (2012). Comment on 'Therapeutic application of metallic nanoparticles combined with particle-induced x-ray emission effect'. Nanotechnology, 23(7), 078002–078001; author reply 078002.
Résumé: A recent paper (Kim et al 2010 Nanotechnology 21 425102) presented results on the combination of irradiation by atomic ions of cells loaded by particles made of heavy atoms. They propose that the projectile induced x-rays emission (PIXE) mechanism has an important contribution to the enhancement of the cell death rate. Experiments made in our group to study the effects of such a combination have shown that the Auger effect induced in the high-Z atoms and the following induction of surrounding water radiolysis has an important contribution to the enhancement of the cell death rate. In the light of our studies we propose an alternative interpretation of the results presented in the paper by Kim et al.
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Lebech, M., Houver, J. C., Raseev, G., dos Santos, A. S., Dowek, D., & Lucchese, R. R. (2012). Valence and inner-valence shell dissociative photoionization of CO in the 26-33 eV range. II. Molecular-frame and recoil-frame photoelectron angular distributions. JOURNAL OF CHEMICAL PHYSICS, 136(9), 094303.
Résumé: Experimental and theoretical results for molecular-frame photoemission are presented for inner-valence shell photoionization of the CO molecule induced by linearly and circularly polarized light. The experimental recoil frame photoelectron angular distributions (RFPADs) obtained from dissociative photoionization measurements where the velocities of the ionic fragment and photoelectron were detected in coincidence, are compared to RFPADs computed using the multichannel Schwinger configuration interaction method. The formalism for including a finite lifetime of the predissociative ion state is presented for the case of general elliptically polarized light, to obtain the RFPAD rather than the molecular frame photoelectron angular distribution (MFPAD), which would be obtained with the assumption of instantaneous dissociation. We have considered photoionization of CO for the photon energies of 26.0 eV, 29.5 eV, and 32.5 eV. A comparison of experimental and theoretical RFPADs allows us to identify the ionic states detected in the experimental studies. In addition to previously identified states, we found evidence for the 2 (2)Delta state with an ionization potential of 25.3 eV and (2)Sigma(+) states with ionization potentials near 32.5 eV. A comparison of the experimental and theoretical RFPADs permits us to estimate predissociative lifetimes of 0.25-1 ps for some of the ion states. Consideration of the MFPADs of a series of (2)Pi ion states indicates the importance of inter-channel coupling at low photoelectron kinetic energy and the limitations of a single-channel analysis based on the corresponding Dyson orbitals. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.3681920]
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Lefebvre, R., Jaouadi, A., & Atabek, O. (2012). Clusters of exceptional points for a laser control of selective vibrational transfer. Chemical Physics, 399, 111.
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Li, C., Casagrande, E. M. S., Lahmam-Bennani, A., & Naja, A. (2012). Identification of first order and non-first order contributions in the (e,3-1e) and (e,3e) double ionization of molecular nitrogen. JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 45(13), 135201.
Résumé: Double ionization of nitrogen molecules is investigated in coplanar asymmetric (e,3-1e) and (e,3e) experiments. The measurements are performed at intermediate incident energy (similar to 600 eV) with one fast scattered electron and two slower ejected electrons sharing equally the excess energy. The data are compared with the predictions of a simple kinematical model recently reported by Lahmam-Bennani et al (2010 J. Phys. B: At. Mol. Opt. Phys. 43 105201) which describes the 'two-step 2' (TS2) mechanism as two successive (e,2e) single ionization interactions. The model is extended to include binary as well as recoil scattering during the two successive single ionization events. It is shown to qualitatively predict the correct angular positions for most of the observed structures. Moreover, the (e,3e) data are compared with the predictions of a first Born model which fails to reproduce the experimental angular distributions. These results demonstrate that the molecular double ionization process is largely dominated by the TS2 mechanism, as was the case in our previous works on atomic targets.
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Lozada-Garcia, R. R., Ceponkus, J., Chevalier, M., Chin, W., Mestdagh, J. - M., & Crepin, C. (2012). Nuclear Spin Conversion to Probe the Methyl Rotation Effect on Hydrogen-Bond and Vibrational Dynamics. Angewandte Chemie-International Edition, 51(28), 6947–6950.
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Lozada-Garcia, R. R., Ceponkus, J., Chevalier, M., Chin, W., Mestdagh, J. - M., & Crepin, C. (2012). Photochemistry of acetylacetone isolated in parahydrogen matrices upon 266 nm irradiation. Physical Chemistry Chemical Physics, 14(10), 3450–3459.
Résumé: The photochemistry of the chelated enol form of acetylacetone (AcAc) was investigated by UV excitation of the S2 state at 266 nm in parahydrogen matrices, complemented by experiments in neon and normal hydrogen matrices. Infrared (IR) spectroscopy, combined with theoretical calculations, was used to identify the photoproducts. Isomerization towards various non-chelated forms (no intramolecular H-bond) of AcAc is the dominant channel whereas fragmentation is very minor. The isomerization kinetics is monitored by IR spectroscopy. Among the seven non-chelated conformers of AcAc, only three are formed in parahydrogen matrices, whereas four are observed in normal hydrogen matrices. This difference suggests that an active tunnelling process between conformers occurs in parahydrogen but is quenched in normal hydrogen where guest-host interactions are stronger. Fragmentation and isomerization of excited AcAc are discussed in the light of these new data. The role of the intermediate triplet state in the S-2 -> S-0 relaxation is confirmed, as the importance of phonons in the condensed phase.
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Makhlouf, H., Perronet, K., Dupuis, G., Leveque-Fort, S., & Dubois, A. (2012). Simultaneous optically sectioned fluorescence and optical coherence microscopy with full-field illumination. OPTICS LETTERS, 37(10), 1613–1615.
Résumé: Full-field optical coherence microscopy (FF-OCM) and optically sectioned fluorescence microscopy are two imaging techniques that are implemented here in a novel dual modality instrument. The two imaging modalities use a broad field illumination to acquire the entire field of view without raster scanning. Optical sectioning is achieved in both imaging modalities owing to the coherence gating property of light for FF-OCM, and a structured illumination setup for fluorescence microscopy. Complementary image data are provided by the dual modality instrument in the context of biological tissue screening. FF-OCM imaging modality shows the tissue microarchitecture, while fluorescence microscopy highlights specific tissue features with cellular-level resolution by using targeting contrast agents. Complementary tissue morphology and biochemical features could potentially improve the understanding of cellular functions and disease diagnosis. (C) 2012 Optical Society of America
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Malis, M., Loquais, Y., Gloaguen, E., Biswal, H. S., Piuzzi, F., Tardivel, B., Brenner, V., Broquier, M., Jouvet, C., Mons, M., Doslic, N., & Ljubic, I. (2012). Unraveling the mechanisms of nonradiative deactivation in model peptides following photoexcitation of a phenylalanine residue. J Am Chem Soc, 134(50), 20340–20351.
Résumé: The mechanisms of nonradiative deactivation of a phenylalanine residue after near-UV photoexcitation have been investigated in an isolated peptide chain model (N-acetylphenylalaninylamide, NAPA) both experimentally and theoretically. Lifetime measurements at the origin of the first pipi* state of jet-cooled NAPA molecules have shown that (i) among the three most stable conformers of the molecule, the folded conformer NAPA B is approximately 50-times shorter lived than the extended major conformer NAPA A and (ii) this lifetime is virtually insensitive to deuteration at the NH(2) and NH sites. Concurrent time-dependent density functional theory (TDDFT) based nonadiabatic dynamics simulations in the full dimensionality, carried out for the NAPA B conformer, provided direct insights on novel classes of ultrafast deactivation mechanisms, proceeding through several conical intersections and leading in fine to the ground state. These mechanisms are found to be triggered either (i) by a stretch of the N(Phe)H bond, which leads to an H-transfer to the ring, or (ii) by specific backbone amide distortions. The potential energy surfaces of the NAPA conformers along these critical pathways have been characterized more accurately using the coupled cluster doubles (CC2) method and shown to exhibit barriers that can be overcome with moderate excess energies. These results analyzed in the light of the experimental findings enabled us to assign the short lifetime of NAPA B conformer to a number of easily accessible exit channels from the initial pipi* surface, most importantly the one involving a transfer of electronic excitation to an npi* surface, induced by distortions of the backbone peptide bond.
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Marinica, D. C., Kazansky, A. K., Nordlander, P., Aizpurua, J., & Borisov, A. G. (2012). Quantum Plasmonics: Nonlinear Effects in the Field Enhancement of a Plasmonic Nanoparticle Dimer. Nano Lett., 12(3), 1333–1339.
Résumé: A fully quantum mechanical investigation using time-dependent density functional theory reveals that the field enhancement in a coupled nanoparticle dimer can be strongly affected by nonlinear effects. We show that both classical as well as linear quantum mechanical descriptions of the system fail even for moderate incident light intensities. An interparticle current resulting from the strong field photo emission tends to neutralize the plasmon-induced surface charge densities on the opposite sides of the nanoparticle junction. Thus, the coupling between the two nanoparticles and the field enhancement is reduced as compared to linear theory. A substantial nonlinear effect is revealed already at incident powers of 10(9) W/cm(2) for interparticle separation distances as large as 1 nm and down to the touching limit.
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Marquer, C., Devauges, V., Cossec, J. - C., Liot, G., Lecart, S., Saudou, F., Duyckaerts, C., Leveque-Fort, S., & Potier, M. - C. (2012). Local cholesterol increase triggers amyloid precursor protein-Bace1 clustering in lipid rafts and rapid endocytosis (vol 25, pg 1295, 2011). FASEB JOURNAL, 26(1), 468.
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Marquer, C., Leveque-Fort, S., & Potier, M. - C. (2012). Determination of lipid raft partitioning of fluorescently-tagged probes in living cells by Fluorescence Correlation Spectroscopy (FCS). Journal of visualized experiments : JoVE, (62), e3513.
Résumé: In the past fifteen years the notion that cell membranes are not homogenous and rely on microdomains to exert their functions has become widely accepted. Lipid rafts are membrane microdomains enriched in cholesterol and sphingolipids. They play a role in cellular physiological processes such as signalling, and trafficking but are also thought to be key players in several diseases including viral or bacterial infections and neurodegenerative diseases. Yet their existence is still a matter of controversy. Indeed, lipid raft size has been estimated to be around 20 nm, far under the resolution limit of conventional microscopy (around 200 nm), thus precluding their direct imaging. Up to now, the main techniques used to assess the partition of proteins of interest inside lipid rafts were Detergent Resistant Membranes (DRMs) isolation and co-patching with antibodies. Though widely used because of their rather easy implementation, these techniques were prone to artefacts and thus criticized. Technical improvements were therefore necessary to overcome these artefacts and to be able to probe lipid rafts partition in living cells. Here we present a method for the sensitive analysis of lipid rafts partition of fluorescently-tagged proteins or lipids in the plasma membrane of living cells. This method, termed Fluorescence Correlation Spectroscopy (FCS), relies on the disparity in diffusion times of fluorescent probes located inside or outside of lipid rafts. In fact, as evidenced in both artificial membranes and cell cultures, probes would diffuse much faster outside than inside dense lipid rafts. To determine diffusion times, minute fluorescence fluctuations are measured as a function of time in a focal volume (approximately 1 femtoliter), located at the plasma membrane of cells with a confocal microscope (Fig. 1). The auto-correlation curves can then be drawn from these fluctuations and fitted with appropriate mathematical diffusion models. FCS can be used to determine the lipid raft partitioning of various probes, as long as they are fluorescently tagged. Fluorescent tagging can be achieved by expression of fluorescent fusion proteins or by binding of fluorescent ligands. Moreover, FCS can be used not only in artificial membranes and cell lines but also in primary cultures, as described recently. It can also be used to follow the dynamics of lipid raft partitioning after drug addition or membrane lipid composition change.
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Martin-Drumel, M. A., Eliet, S., Pirali, O., Guinet, M., Hindle, F., Mouret, G., & Cuisset, A. (2012). New investigation on THz spectra of OH and SH radicals (X-2 Pi(i)). CHEMICAL PHYSICS LETTERS, 550, 8–14.
Résumé: Pure rotational transitions of OH and SH radicals have been recorded in the THz spectral range using cw-THz and synchrotron-based FT-FIR techniques. Line lists on these radicals have been completed in the three and two lowest vibrational states for OH and SH, respectively. Furthermore, the hyperfine structure of OH and SH has been observed for the first time using infrared IR FT-spectroscopy, and at frequencies higher than 1 THz, respectively. A combined fit has been made for each of these radicals including v = 0, 1 and 2 for OH and v = 0 and 1 for SH. (c) 2012 Elsevier B.V. All rights reserved.
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Mendes, L. A. V., Boye-Peronne, S., Jacovella, U., Lievin, J., & Gauyacq, D. (2012). Rydberg states of cyanoacetylene investigated by (3+1) REMPI spectroscopy in the 77,000-90,000 cm(-1) energy range. MOLECULAR PHYSICS, 110(21-22), 2829–2842.
Résumé: (3 + 1) resonantly enhanced multiphoton ionization (REMPI) spectroscopy coupled to photoelectron spectroscopy (REMPI-PES) has been carried out to study the Rydberg states of HC3N in the 77,000-90,000 cm(-1) region. Ab initio calculations (energies and optimized equilibrium geometries) have been performed for the first time for the low-lying (X) over tilde (2)Pi, (A) over tilde (2)Sigma(+) and (B) over tilde (2)Pi states of the cation HC3N+ in order to help the analysis. Thanks to the combination of the three-photon REMPI spectra, one-photon spectrum and photoelectron spectra, unambiguous assignments of the Rydberg series and their vibrationally excited members are proposed. The electronic Rydberg structure of cyanoacetylene is very similar to that of C2H2 and HCN (almost identical quantum defects), fully supporting the present analysis. New three-photon allowed Rydberg series are identified belonging to ns and nd series. The three-photon vibrational band assignments, confirmed by the photoelectrons spectra, reveal excitation of only one or two quanta of the nu(2) (C N) mode. Apparent discrepancies between the three-photon REMPI spectrum and the one-photon absorption spectrum are removed via a minor re-assignment of the absorption spectrum previously analysed by Connors et al. J. Chem. Phys. 60(12), 5011 (1974). Finally the observed analogy with C2H2 and HCN can be rationalized by a partial relocalization of the 2 pi electrons upon excitation to Rydberg states converging to the (X) over tilde (2)Pi state of HC3N+, as predicted by the present ab initio calculations on the cation core.
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Meng, L., Bourgaux, A. - C., Bastiani-Ceccotti, S., Guilbaud, O., Pittman, M., Kazamias, S., Cassou, K., Daboussi, S., Ros, D., & Klisnick, A. (2012). Temporal characterization of a picosecond extreme ultraviolet laser pumped in grazing incidence. APPLIED PHYSICS LETTERS, 101(14), 141125.
Résumé: We report an experimental study of the temporal duration of a transient pumping extreme ultraviolet (XUV) laser emitted at 18.9 nm, using an ultrafast x-ray streak camera. We have investigated the shot-to-shot reproducibility of the pulse duration, as well as its behaviour as a function of several pumping parameters. Our results show that the pulse duration increases slowly with the pump pulse duration, in agreement with previous observations performed in a different geometry. The angle of the pump laser relative to the target surface also affects the XUV laser duration in a measurable way. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4757878]
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Nguyen-Thi Van-Oanh, Falvo, C., Calvo, F., Lauvergnat, D., Basire, M., Gaigeot, M. - P., & Parneix, P. (2012). Improving anharmonic infrared spectra using semiclassically prepared molecular dynamics simulations. PHYSICAL CHEMISTRY CHEMICAL PHYSICS, 14(7), 2381–2390.
Résumé: Classical molecular dynamics is a convenient method for computing anharmonic infrared spectra of polyatomic molecules and condensed phase systems. However it does not perform well for predicting accurate intensities and it lacks nuclear quantization, two deficiencies that are usually accounted for by empirical scaling factors. In this paper we show on the examples of the trans isomer of nitrous acid and naphthalene that both issues can be alleviated by preparing the initial conditions according to semiclassical quantization based on a normal mode representation. The method correctly reproduces fundamental frequencies obtained with quantum mechanical methods. At increasing temperatures, the effective frequencies are found to follow the same trends as path-integral based methods. In the low-temperature limit, the band intensities predicted by the method are also found to agree with quantum mechanical considerations.
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Nimmrich, M., Kittelmann, M., Rahe, P., Harneit, W., Mayne, A. J., Dujardin, G., & Kuhnle, A. (2012). Influence of charge transfer doping on the morphologies of C-60 islands on hydrogenated diamond C(100)-(2 x 1). Phys. Rev. B, 85(3), 035420.
Résumé: The adsorption and island formation of C-60 fullerenes on the hydrogenated C(100)-(2 x 1):H diamond surface is studied using high-resolution noncontact atomic force microscopy in ultrahigh vacuum. At room temperature, C-60 fullerene molecules assemble into monolayer islands, exhibiting a hexagonally close-packed internal structure. Dewetting is observed when raising the substrate temperature above approximately 505 K, resulting in two-layer high islands. In contrast to the monolayer islands, these double-layer islands form extended wetting layers. This peculiar behavior is explained by an increased molecule-substrate binding energy in the case of double-layer islands, which originates from charge transfer doping. Only upon further increasing the substrate temperature to approximately 615 K, the wetting layer desorbs, corresponding to a binding energy of the charge transfer-stabilized film of 1.7 eV.
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Parneix, P., Basire, M., & Calvo, F. (2012). Time-resolved infrared emission spectra of naphthalene under gas phase laboratory and astrophysical conditions. COMPUTATIONAL AND THEORETICAL CHEMISTRY, 990, 112–118.
Résumé: The relaxation of neutral naphthalene C10H8 upon electronic excitation is theoretically modeled as a function of time by considering infrared emission cascade in competition with statistical dissociation, within the framework of kinetic Monte Carlo simulations. The possible importance of collisional energy transfer with a surrounding low-density medium is evaluated, and shown to agree with existing measurements. (C) 2011 Elsevier B.V. All rights reserved.
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Peters, M., Nguyen-Dang, T. T., Charron, E., Keller, A., & Atabek, O. (2012). Laser-induced electron diffraction: A tool for molecular orbital imaging. PHYSICAL REVIEW A, 85(5), 053417.
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Pirali, O., Boudon, V., Oomens, J., & Vervloet, M. (2012). Rotationally resolved infrared spectroscopy of adamantane. JOURNAL OF CHEMICAL PHYSICS, 136(2), 024310.
Résumé: We present the first rotationally resolved spectra of adamantane (C(10)H(16)) applying gas-phase Fourier transform infrared (IR) absorption spectroscopy. High-resolution IR spectra are recorded in the 33-4500 cm(-1)range using as source of IR radiation both synchrotron radiation (at the AILES beamline of the SOLEIL synchrotron) as well as a classical globar. Adamantane is a spherical top molecule with tetrahedral symmetry (T(d) point group) and has no permanent dipole moment in its vibronic ground state. Of the 72 fundamental vibrational modes in adamantane, only 11 are IR active. Here we present rotationally resolved spectra for seven of them: nu(30), nu(28), nu(27), nu(26), nu(25), nu(24), and nu(23). The typical rotational structure of spherical tops is observed and analyzed using the STDS software developed in the Dijon group, which provides the first accurate energy levels and rotational constants for seven fundamental modes. Rotational levels with quantum numbers as high as J = 107 have been identified and included in the fit leading to a typical standard deviation of about 10(-3) cm(-1).
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Prato, M., Toccafondi, C., Maidecchi, G., Chaudhari, V., Harish, M. N. K., Sampath, S., Parodi, R., Esaulov, V. A., & Canepa, M. (2012). Mercury Segregation and Diselenide Self-Assembly on Gold. JOURNAL OF PHYSICAL CHEMISTRY C, 116(3), 2431–2437.
Résumé: We have investigated the self-assembly of didecyldiselenide on gold containing mercury using X-ray photoelectron spectroscopy, cyclic voltammetry and infrared spectroscopy. The analysis of intensity and chemical shift of selected Se, Hg, and Au photoelectron lines on samples with increasing Hg content, show that didecyldiselenide adsorption strongly contributed to segregation of bulk Hg to the surface. The voltammetry results support this conclusion and suggest the formation of Hg-Au surface amalgam. The Hg surface segregation effect must be related to the restructuring of the surface following initial adsorption, and to the strong selenophilicity of Hg. The reflectance absorbance infrared spectroscopy studies show that the molecular layer on Hg-Au substrates lacks good order.
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Quirico, E., Orthous-Daunay, F. - R., Bonal, L., Beck, P., Schmitt, B., Brunetto, R., Dartois, E., Pino, T., Engrand, C., & Duprat, J. (2012). THE MULTIPLE ORIGINS OF INSOLUBLE ORGANIC MATTER FROM PRIMITIVE CHONDRITES. METEORITICS & PLANETARY SCIENCE, 47, A323.
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Raseev, G. (2012). Laser fields at flat interfaces: I. Vector potential. Eur. Phys. J. D, 66(7), 179.
Résumé: A model calculating the laser fields at a flat structureless surface taking into account the surface photoelectric effect is presented. The photon is p or transverse magnetic linearly polarized, continuous and its wave length is long, i.e. lambda(vac) >= 12.4 nm. The sharp rise of the electron density at the interface generates an atomic scale spatial dependence of the laser field. In real space and in the temporal gauge, the vector potential A of the laser is obtained as a solution of the classical Ampere-Maxwell and the material equations. The susceptibility is a product of the electron density of the material system with the surface and of the bulk tensor and non-local isotropic (TNLI) polarizability. The electron density is obtained quantum mechanically by solving the Schrodinger equation. The bulk TNLI polarizability including dispersion is calculated from a Drude-Lindhard-Kliewer model. In one dimension perpendicular to the surface the components A(x)(z,omega) and A(z)(z,omega) of the vector potential are solutions of the Ampere-Maxwell system of two coupled integro-differential equations. The model, called vector potential from the electron density-coupled integro-differential equations (VPED-CIDE), is used here to obtain the electron escape probability from the power density absorption, the reflectance, the electron density induced by the laser and Feibelman's parameters d(parallel to) and d(perpendicular to). Some preliminary results on aluminium surfaces are given here and in a companion paper the photoelectron spectra are calculated with results in agreement with the experiment.
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Raseev, G. (2012). Laser fields at flat interfaces: II. Plasmon resonances in aluminium photoelectron spectra. Eur. Phys. J. D, 66(7), 180.
Résumé: Using the model derived in paper I [G. Raseev, Eur. Phys. J. D 66, 167 (2012)], this work presents calculations of the photoelectron spectrum (PES) of low index aluminium surfaces in the 10-30 eV region. The laser is p or transverse magnetic linearly polarized incident on a flat structureless surface and its fields are modeled in I using the vector potential in the temporal gauge. This model uses a tensor and nonlocal isotropic (TNLI) susceptibility and solves the classical Ampere-Maxwell equation through the use of the vector potential from the electron density-coupled integro-differential equations (VPED-CIDE). The PE cross sections are the squares of the PE transition moments calculated using the VPED-CIDE vector potential function of the penetration coordinate. The PES is obtained in a one step model using either the Fermi golden rule or the Weisskopf-Wigner (WW) expressions. The WW cross section PES compares favorably with the experimental angle and energy resolved photoelectron yield (AERPY) spectrum of Levinson et al. [Phys. Rev. Lett. 43, 952 (1979)], Levinson and Plummer [Phys. Rev. B 24, 628 (1981)] for Al(001) and of Barman et al. [Phys. Rev. B 58, R4285 (1998)], Barman [Curr. Sci. 88, 54 (2005)] for Al(111) surfaces. As in the experiment, our theoretical AERPY displays the multipole surface plasmon resonance at 11.32/12.75 eV for Al(001)/Al(111), mainly due to the surface contribution vertical bar <psi(f)vertical bar p . A vertical bar psi(i)>vertical bar(2), the bulk plasmon minimum at 15 eV and the two single particle excitation resonances at about 16 and 22 eV. The nature of the plasmon resonances of the PES is analyzed using the reflectance, the electron density induced by the laser and Feibelman's parameter d(perpendicular to) all introduced in paper I.
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Richardson, V., Li, W. B., Kelly, T. J., Costello, J. T., Nikolopoulos, L. A. A., Duesterer, S., Cubaynes, D., & Meyer, M. (2012). Dichroism in the above-threshold two-colour photoionization of singly charged neon. JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 45(8), 085601.
Résumé: In this work we report on the ionization of a gaseous neon target by combining extreme ultraviolet (XUV) radiation from the Free Electron Laser in Hamburg with an intense synchronized optical laser. Applying energy-resolved photoelectron spectroscopy, the dependence of the electrons ejected from singly charged neon (Ne+) on the relative polarization of the XUV and optical laser fields was investigated. The electron spectra exhibit a strong dependence on the degree of the relative orientation of the linear polarization vectors. A quantitative analysis was undertaken using multichannel time-dependent perturbation theory in order to reproduce the magnitude of the ejected low kinetic energy electrons as a function of the relative polarization directions and explicitly taking into account the influence of the residual Ne2+ cores (D-1, P-3). It is concluded that the variation of the photoelectron spectrum with the deviation of XUV and optical field directions is mainly related to the different responses of the magnetic substates of the ejected electrons in their interaction with the laser field.
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Sanzharov, M., Vander Auwera, J., Pirali, O., Roy, P., Brubach, J. - B., Manceron, L., Gabard, T., & Boudon, V. (2012). Self and N-2 collisional broadening of far-infrared methane lines measured at the SOLEIL synchrotron. JOURNAL OF QUANTITATIVE SPECTROSCOPY & RADIATIVE TRANSFER, 113(15), 1874–1886.
Résumé: Following our recent study devoted to measurements of intensities of pure rotation lines of methane, room temperature far infrared spectra of methane diluted in nitrogen at five total pressures between 100 and 800 hPa have been recorded at the AILES beamline of the SOLEIL synchrotron. One hundred and five N-2 broadening coefficients of methane pure rotation lines have been measured in the 83-261 cm(-1) spectral range using multi-spectrum non-linear least squares fitting of Voigt profiles. Pressure-induced line shifts were not needed to fit the spectra to the noise level and line mixing effects were neglected. One hundred and seventy-six self broadening coefficients have also been measured in the 59-288 cm(-1) spectral range using the pure methane spectra recorded in our previous work. The measured N-2 broadening coefficients were compared to semi-classical calculations. (C) 2012 Elsevier Ltd. All rights reserved.
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Sarsa, A., & Le Sech, C. (2012). Quantum confinement study of the H-2(+) ion with the Monte Carlo approach. Respective role of electron and nuclei confinement. JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 45(20), 205101.
Résumé: A simple approximate trial wavefunction is used to study, within a variational approach and beyond the Born-Oppenheimer approximation, the molecular ion H-2(+) confined by impenetrable spherical surfaces. This wavefunction describes explicitly the motion of the nuclei and the electron of this three-body system in its lowest rovibrational state. Two cut-off functions are introduced to fulfil the Dirichlet boundary conditions, respectively, for the electron and the nuclei. The results show an increase of the energy of the ion when both the confinement radius r(ce) of the electron and R-cN of the nuclei become smaller. The electron constraint is found to be much more efficient to increase the energy than the nuclei confinement. This study shows that a metastable bound state of the ion, above the energy corresponding to the dissociation limit, can be obtained when the electron constraint is present. Expectation values of the internuclear and electron-to-origin distances are also calculated and show a rapid decrease when the confinement is stronger. Finally, the quantum pressure versus the confinement radius is also estimated. A rapid rise of the pressure value when r(ce) is less than 3 au is observed.
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Savage, K. J., Hawkeye, M. M., Esteban, R., Borisov, A. G., Aizpurua, J., & Baumberg, J. J. (2012). Revealing the quantum regime in tunnelling plasmonics. Nature, 491(7425), 574–577.
Résumé: When two metal nanostructures are placed nanometres apart, their optically driven free electrons couple electrically across the gap. The resulting plasmons have enhanced optical fields of a specific colour tightly confined inside the gap. Many emerging nanophotonic technologies depend on the careful control of this plasmonic coupling, including optical nanoantennas for high-sensitivity chemical and biological sensors(1), nanoscale control of active devices(2-4), and improved photovoltaic devices(5). But for subnanometre gaps, coherent quantum tunnelling becomes possible and the system enters a regime of extreme non-locality in which previous classical treatments(6-14) fail. Electron correlations across the gap that are driven by quantum tunnelling require a new description of non-local transport, which is crucial in nanoscale optoelectronics and single-molecule electronics. Here, by simultaneously measuring both the electrical and optical properties of two gold nanostructures with controllable subnanometre separation, we reveal the quantum regime of tunnelling plasmonics in unprecedented detail. All observed phenomena are in good agreement with recent quantum-based models of plasmonic systems(15), which eliminate the singularities predicted by classical theories. These findings imply that tunnelling establishes a quantum limit for plasmonic field confinement of about 10(-8) lambda(3) for visible light (of wavelength lambda). Our work thus prompts new theoretical and experimental investigations into quantum-domain plasmonic systems, and will affect the future of nanoplasmonic device engineering and nanoscale photochemistry.
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Savee, J. D., Soorkia, S., Welz, O., Selby, T. M., Taatjes, C. A., & Osborn, D. L. (2012). Absolute photoionization cross-section of the propargyl radical. J. Chem. Phys., 136(13), 134307.
Résumé: Using synchrotron-generated vacuum-ultraviolet radiation and multiplexed time-resolved photoionization mass spectrometry we have measured the absolute photoionization cross-section for the propargyl (C(3)H(3)) radical, sigma(propargyl) (ion)(E), relative to the known absolute cross-section of the methyl (CH(3)) radical. We generated a stoichiometric 1:1 ratio of C(3)H(3):CH(3) from 193 nm photolysis of two different C(4)H(6) isomers (1-butyne and 1,3-butadiene). Photolysis of 1-butyne yielded values of sigma(propargyl)(ion)(10.213 eV)=(26.1+/-4.2) Mb and sigma(propargyl)(ion)(10.413 eV)=(23.4+/-3.2) Mb, whereas photolysis of 1,3-butadiene yielded values of sigma(propargyl)(ion)(10.213 eV)=(23.6+/-3.6) Mb and sigma(propargyl)(ion)(10.413 eV)=(25.1+/-3.5) Mb. These measurements place our relative photoionization cross-section spectrum for propargyl on an absolute scale between 8.6 and 10.5 eV. The cross-section derived from our results is approximately a factor of three larger than previous determinations.
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Schliesser, A., Picque, N., & Haensch, T. W. (2012). Mid-infrared frequency combs. NATURE PHOTONICS, 6(7), 440–449.
Résumé: Laser frequency combs are coherent light sources that emit a broad spectrum of discrete, evenly spaced narrow lines whose absolute frequency can be measured to within the accuracy of an atomic clock. Their development in the near-infrared and visible domains has revolutionized frequency metrology while also providing numerous unexpected opportunities in other fields such as astronomy and attosecond science. Researchers are now exploring how to extend frequency comb techniques to the mid-infrared spectral region. Versatile mid-infrared frequency comb generators based on novel laser gain media, nonlinear frequency conversion or microresonators promise to significantly expand the applications of frequency combs. In particular, novel approaches to molecular spectroscopy in the 'fingerprint region', with dramatically improved precision, sensitivity, recording time and/or spectral bandwidth may lead to new discoveries in the various fields relevant to molecular science.
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Schubert, K., Damm, A., Eremeev, S. V., Marks, M., Shibuta, M., Berthold, W., Guedde, J., Borisov, A. G., Tsirkin, S. S., Chulkov, E. V., & Hoefer, U. (2012). Momentum-resolved electron dynamics of image-potential states on Cu and Ag surfaces. Phys. Rev. B, 85(20), 205431.
Résumé: The dependence of the inelastic lifetime of electrons in the first n = 1 image-potential state of clean and rare-gas covered Ag(111), Cu(111), and Cu(100) surfaces on their momentum parallel to the surface has been studied experimentally by means of time-and angle-resolved two-photon photoemission spectroscopy (2PPE) and theoretically by calculations based on the many-body theory within the self-energy formalism. Similar to the previously studied clean Cu(100) surface, the theoretical results are in excellent agreement with the experiment findings for Cu(111). For Ag(111), the theory overestimates the decay rate and its momentum dependence, which is attributed to the neglect of surface plasmon excitations. With increasing parallel momentum, the n = 1 state shifts out of the projected bulk band gap on both surfaces and turns into an image-potential resonance. This opens an additional decay channel by resonant electron transfer into the bulk, which is theoretically treated by the application of the wave packet propagation approach. The expected stronger increase of the decay rate upon crossing the edge of the band gap, however, is not observed in the experiment. The decoupling of the image-potential states from the metal surface upon adsorption of rare-gas layers results in a decrease of the decay rate as well as of its momentum dependence by a similar factor, which can be successfully explained by the change of interband and intraband contributions to the total decay rate.
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Sen, A., Bouchet, A., Lepere, V., Le Barbu-Debus, K., Scuderi, D., Piuzzi, F., & Zehnacker-Rentien, A. (2012). Conformational Analysis of Quinine and Its Pseudo Enantiomer Quinidine: A Combined Jet-Cooled Spectroscopy and Vibrational Circular Dichroism Study. JOURNAL OF PHYSICAL CHEMISTRY A, 116(32), 8334–8344.
Résumé: Laser-desorbed quinine and quinidine have been studied in the gas phase by combining supersonic expansion with laser spectroscopy, namely, laser-induced fluorescence (LIF), resonance-enhanced multiphoton ionization (REMPI), and IR-UV double resonance experiments. Density functional theory (DFT) calculations have been done in conjunction with the experimental work. The first electronic transition of quinine and quinidine is of pi-pi* nature, and the studied molecules weakly fluoresce in the gas phase, in contrast to what was observed in solution (Qin, W. W.; et al. J. Phys. Chem. C 2009, 113, 11790). The two pseudo enantiomers quinine and quinidine show limited differences in the gas phase; their main conformation is of open type as it is in solution. However, vibrational circular dichroism (VCD) experiments in solution show that additional conformers exist in condensed phase for quinidine, which are not observed for quinine. This difference in behavior between the two pseudo enantiomers is discussed.
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Song, J., Wang, L., Jin, L., Xia, X., Kou, Q., Bouchoule, S., & He, J. - J. (2012). Intensity-Interrogated Sensor Based on Cascaded Fabry-Perot Laser and Microring Resonator. JOURNAL OF LIGHTWAVE TECHNOLOGY, 30(17), 2901–2906.
Résumé: A highly sensitive integrated optical biosensor based on the cascade of a Fabry-Perot cavity laser and a microring resonator is investigated theoretically and experimentally. The free spectral ranges of the microring and the laser cavity are designed to be about the same in order to apply intensity interrogation. The variation of the refractive index of the fluidic sample results in a large shift in the envelope function of the total transmission spectrum of the sensor, and consequently, a large change in the transmitted power. The simple light-source-integrated sensing scheme achieved a high sensitivity of 1000 dB/RIU in the preliminary experiment, demonstrating its principle and potential for low-cost practical applications.
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Soorkia, S., Leone, S. R., & Wilson, K. R. (2012). Radical-neutral chemical reactions studied at low temperature with VUV synchrotron photoionization mass spectrometry. AIP Conference Proceedings, 1501, 1365–1372.
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Spillebout, F., Stauffer, L., Sonnet, P., & Mayne, A. J. (2012). Stability of small chemical groups on hexagonal-SiC(0001) surfaces: A theoretical study. SURFACE SCIENCE, 606(15-16), 1195–1202.
Résumé: Density functional theory (DFT) calculations are used to investigate the stability on SiC(0001) surfaces of different chemical groups -NH2, -NO2, -CH3, -OH, -SH and -CN. The adsorption stability decreases in the order -NO2 > -OH > -NH2 > -SH > -CN > -CH3. The stability of the single molecule-substrate bond is strongly influenced by the polarizability, which in turn depends on different parameters such as the electronegativity, atomic size and chemical environment. In a further step, methyl (-ACH(3)) and phenyl (-AC(6)H(5)) substituted groups are also considered and similar behaviour is observed. The inductive effect of the -CH3 or -C6H5 groups modifies the polarization of the Si adatom-molecule bond and the steric hindrance due to their size influences the molecular orientation. These two parameters affect the calculated adsorption energy, and are more important for -C6H5 substituent. This study provides clear tendencies that can be applied to more complex systems. Comparison of the adsorption of two large molecules, H2Pc (metal-free phthalocyanine) and PTCDI (perylene tetracarboxylic diimide) on the SiC(0001) surface is presented as an example. (C) 2012 Elsevier B.V. All rights reserved.
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Sunil Kumar, S., Lucas, B., Soorkia, S., Barat, M., & Fayeton, J. A. (2012). Calpha-Cbeta chromophore bond dissociation in protonated tyrosine-methionine, methionine-tyrosine, tryptophan-methionine, methionine-tryptophan and their sulfoxide analogs. Phys. Chem. Chem. Phys., 14(29), 10225–32.
Résumé: C(alpha)-C(beta) chromophore bond dissociation in some selected methionine-containing dipeptides induced by UV photons is investigated. In methionine containing dipeptides with tryptophan as the UV chromophore, the tryptophan side chain is ejected either as an ion or as a neutral fragment while in dipeptides with tyrosine, the tyrosine side chain is lost only as a neutral fragment. Mechanisms responsible for these fragmentations are proposed based on measured branching ratios and fragmentation times, and on the results of DFT/B3-LYP calculations. It appears that the C(alpha)-C(beta) bond cleavage is a non-statistical dissociation for the peptides containing tyrosine, and occurs after internal conversion for those with tryptophan. The proposed mechanisms are governed by the ionization potential of the aromatic side chain compared to that of the rest of the molecule, and by the proton affinity of the aromatic side chain compared to that of the methionine side chain. In tyrosine-containing peptides, the presence of oxygen on sulfur of methionine presumably reduces the ionization potential of the peptide backbone, facilitating the loss of the side chain as a neutral fragment. In tryptophan-containing peptides, the presence of oxygen on methionyl-sulfur expedites the transfer of the proton from the side chain to the sulfoxide, which facilitates the loss of the neutral side chain.
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Thibault, F., Gomez, L., Ivanov, S. V., Buzykin, O. G., & Boulet, C. (2012). Comparison of quantum, semi-classical and classical methods in the calculation of nitrogen self-broadened linewidths. JOURNAL OF QUANTITATIVE SPECTROSCOPY & RADIATIVE TRANSFER, 113(15), 1887–1897.
Résumé: We perform dynamical calculations on two robust N-2-N-2 potential energy surfaces in order to intercompare pressure broadening coefficients derived from close coupling and coupled states quantum dynamical methods, the semi-classical model of Robert and Bonamy and a full classical method. The coupled states and full classical results compare well with the experimental results or with close coupling values when available. This study confirms that the classical method is a good alternative at room and high temperatures to quantum dynamical methods. The results obtained using the semi-classical method however deviate from the other sets of data at all temperatures considered here (77-2400 K). (C) 2012 Elsevier Ltd. All rights reserved.
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Tudorie, M., Ilyushin, V., Vander Auwera, J., Pirali, O., Roy, P., & Huet, T. R. (2012). Synchrotron FTIR spectroscopy of weak torsional bands: A case study of cis-methyl formate. JOURNAL OF CHEMICAL PHYSICS, 137(6), 064304.
Résumé: The far infrared spectrum of cis-methyl formate has been recorded on the AILES beamline of the synchrotron SOLEIL using a Fourier transform infrared spectrometer coupled to a long path cell. The very weak fundamental band associated with the methyl-top torsion mode (v(18)) was observed. The frequency analysis was performed using the “rho axis method”, and the microwave and millimeter-wave data from the literature. A precise determination of the band origins (v(18)(A) = 132.4303 cm(-1) and v(18)(E) = 131.8445 cm(-1)) and of the barrier height [V-3 = 370.7398 (58) cm(-1)] have been obtained. The intensity of the v(18) fundamental band was determined to be 3.4 x 10(-21) cm(-1)/(molecule cm(-2)) at 297 K, equally shared among A-A and E-E transitions, thus leading to a dipole moment component mu((3))(c) equal to 0.0483 D. The results were compared with the ab initio calculations of Senent et al. [Astrophys. J. 627, 567 (2005)]. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4740250]
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Turowski, M., Crepin, C., Couturier-Tamburelli, I., Pietri, N., & Kolos, R. (2012). Low-temperature phosphorescence of dicyanoacetylene in rare gas solids. LOW TEMPERATURE PHYSICS, 38(8), 723–726.
Résumé: A strong visible a(similar to 3)Sigma(+)(u) – X-similar to 1 Sigma(+)(g) luminescence was observed upon UV excitation of cryogenic rare gas (argon, krypton, and xenon) matrices doped with dicyanoacetylene (NC4N). Spectra and life-times of this phosphorescence have been measured. A detailed analysis of resolved vibronic bands is presented. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4745884]
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Turowski, M., Crepin, C., Douin, S., Gronowski, M., Couturier-Tamburelli, I., Pietri, N., Wasiak, A., & Kolos, R. (2012). Low temperature Raman spectra of cyanobutadiyne (HC5N). VIBRATIONAL SPECTROSCOPY, 62, 268–272.
Résumé: Low temperature Raman scattering spectra of cyanobutadiyne, either condensed from the vapour as a solid film, or isolated in a cryogenic argon matrix, have been measured – leading to the identification of all vibrational fundamentals, together with several overtones and combination modes. The analysis is based on previous experimental data, including the vibrationally resolved phosphorescence spectra, and on the comparison to available theoretical predictions. (C) 2012 Elsevier B.V. All rights reserved.
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Urbanski, L., Marconi, M. C., Meng, L. M., Berrill, M., Guilbaud, O., Klisnick, A., & Rocca, J. J. (2012). Spectral linewidth of a Ne-like Ar capillary discharge soft-x-ray laser and its dependence on amplification beyond gain saturation. PHYSICAL REVIEW A, 85(3), 033837.
Résumé: We report the measurement of the linewidth and temporal coherence of a lambda=46.9 nm neon-like argon capillary discharge soft-x-ray laser and its variation with plasma column length. A wave-front-division interferometer was used to resolve the 3p S-1(0)-3s P-1(1) laser line, resulting in measured relative linewidths of Delta lambda/lambda = (3-4) x 10(-5). The measurements do not observe saturation rebroadening when this clearly dominantly Doppler-broadened inhomogeneous line is amplified beyond the intensity corresponding to gain saturation. Model simulations indicate this is the result of a comparatively small collisional broadening that sufficiently homogenizes the line profile to practically eliminate inhomogeneous saturation rebroadening. Collisional redistribution is computed to play only a very minor role in homogenizing the line profile.
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Wakelam, V., Herbst, E., Loison, J. - C., Smith, I. W. M., Chandrasekaran, V., Pavone, B., Adams, N. G., Bacchus-Montabonel, M. - C., Bergeat, A., Beroff, K., Bierbaum, V. M., Chabot, M., Dalgarno, A., van Dishoeck, E. F., Faure, A., Geppert, W. D., Gerlich, D., Galli, D., Hebrard, E., Hersant, F., Hickson, K. M., Honvault, P., Klippenstein, S. J., Le Picard, S., Nyman, G., Pernot, P., Schlemmer, S., Selsis, F., Sims, I. R., Talbi, D., Tennyson, J., Troe, J., Wester, R., & Wiesenfeld, L. (2012). A KINETIC DATABASE FOR ASTROCHEMISTRY (KIDA). ASTROPHYSICAL JOURNAL SUPPLEMENT SERIES, 199(1), 21.
Résumé: We present a novel chemical database for gas-phase astrochemistry. Named the KInetic Database for Astrochemistry (KIDA), this database consists of gas-phase reactions with rate coefficients and uncertainties that will be vetted to the greatest extent possible. Submissions of measured and calculated rate coefficients are welcome, and will be studied by experts before inclusion into the database. Besides providing kinetic information for the interstellar medium, KIDA is planned to contain such data for planetary atmospheres and for circumstellar envelopes. Each year, a subset of the reactions in the database (kida.uva) will be provided as a network for the simulation of the chemistry of dense interstellar clouds with temperatures between 10 K and 300 K. We also provide a code, named Nahoon, to study the time-dependent gas-phase chemistry of zero-dimensional and one-dimensional interstellar sources.
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Westover, J., Enriquez, H., Oughaddou, H., & Kara, A. (2012). Metallization of the beta-SiC(100) 3x2 surface: A DFT investigation. SURFACE SCIENCE, 606(19-20), 1471–1474.
Résumé: Using density functional theory (DFT) we report results for the electronic structure and vibrational dynamics of hydrogenated silicon carbide (001) (3 x 2) surfaces with various levels of hydrogenation. These results were obtained using density functional theory with a generalized gradient exchange correlation function. The calculations reveal that metallization can be achieved via hydrogen atoms occupying the second silicon layer. Further increase of hydrogen occupation on the second silicon layer sites results in a loss of this metallization. For the former scenario, where metallization occurs, we found a new vibrational mode at 1870 cm(-1), which is distinct from the mode associated with hydrogen atoms on the first layer. Furthermore, we found the diffusion barrier for a hydrogen atom to move from the second to the third silicon layer to be 258 meV. (c) 2012 Elsevier B.V. All rights reserved.
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Yang, H., Boudrioua, O., Mayne, A. J., Comtet, G., Dujardin, G., Kuk, Y., Sonnet, P., Stauffer, L., Nagarajan, S., & Gourdon, A. (2012). The paradox of an insulating contact between a chemisorbed molecule and a wide band gap semiconductor surface. Phys. Chem. Chem. Phys., 14(5), 1700–1705.
Résumé: Controlling the intrinsic optical and electronic properties of a single molecule adsorbed on a surface requires electronic decoupling of some molecular orbitals from the surface states. Scanning tunneling microscopy experiments and density functional theory calculations are used to study a perylene molecule derivative (DHH-PTCDI), adsorbed on the clean 3 x 3 reconstructed wide band gap silicon carbide surface (SiC(0001)-3 x 3). We find that the LUMO of the adsorbed molecule is invisible in I(V) spectra due to the absence of any surface or bulk states and that the HOMO has a very low saturation current in I(z) spectra. These results present a paradox that the molecular orbitals are electronically isolated from the surface of the wide band gap semiconductor even though strong chemical bonds are formed.
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Yu, S. S., Pearson, J. C., Drouin, B. J., Martin-Drumel, M. A., Pirali, O., Vervloet, M., Coudert, L. H., Muller, H. S. P., & Brunken, S. (2012). Measurement and analysis of new terahertz and far-infrared spectra of high temperature water. JOURNAL OF MOLECULAR SPECTROSCOPY, 279, 16–25.
Résumé: Terahertz absorption spectroscopy and far infrared Fourier transform (FIR-FT) emission spectroscopy were employed to measure new rotational and ro-vibrational spectra and validate existing datasets for high temperature water, with the goal to improve the accuracy of predictions for pure rotation in the (0 2 0), (1 0 0) and (0 0 1) vibrational states. A total of 104 new rotational transitions in (0 0 0), (0 1 0), (0 2 0), (1 0 0) and (0 0 1) were observed in the 293-2723 GHz region with MW accuracy and with observed J(Max) = 18, 11, 10, 14, 10; K-a(Max)= 10, 7, 7, 7, 4; E ''(Max)= 4178, 3771, 4996, 5430, 4939 cm(-1), respectively. A total of 4194 new FIR-FT transitions were assigned in the 50-600 cm(-1) region to the same five vibrational states with estimated experimental uncertainty of 0.0008-0.002 cm(-1) and with J(Max) = 27; K-a(Max) = 21, 18, 18, 17, 17, respectively. Together with previous high-resolution observations, these new data were fitted with the Bending-Rotation approach and the Euler Hamiltonian. The new measurements and predictions reported here will support the analyses of astronomical observations by high-resolution spectroscopy telescopes such as Herschel, SOFIA, and ALMA. (c) 2012 Elsevier Inc. All rights reserved.
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Zugarramurdi, A., & Borisov, A. G. (2012). Transition from fast to slow atom diffraction. Phys. Rev. A, 86(6), 062903.
Résumé: For energetic atomic beams grazingly incident at a surface along low-index directions, the fast motion of the projectile in the surface plane and the slow motion in the direction perpendicular to the surface appear nearly decoupled. Fast-atom diffraction (FAD) experiments reveal two-dimensional (2D) diffraction patterns associated with exchange of the reciprocal vector perpendicular to the low-index direction of fast motion. These results are usually interpreted within the axial-channeling approximation, where the effective 2D potential experienced by the projectile is set as an average of the 3D surface potential along the atomic strings forming the channel. In this work, using the example of grazing scattering of He atoms at a LiF(001) surface, we address theoretically the range of validity of the axial-channeling approximation. Full quantum wave-packet-propagation calculations are used to study the transition from the 2D (fast atom) to the 3D diffraction pattern characteristic for low-energy atomic and molecular projectiles scattered from surfaces. Along with exact calculations, a semianalytical perturbative treatment based on the Lippmann-Schwinger equation allows an explanation of why the diffraction processes involving the exchange of reciprocal-lattice vectors along the fast-motion direction are exponentially small in typical FAD conditions.
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Zugarramurdi, A., Zabala, N., Silkin, V. M., Chulkov, E. V., & Borisov, A. G. (2012). Quantum-well states with image state character for Pb overlayers on Cu(111). Phys. Rev. B, 86(7), 075434.
Résumé: We study theoretically the quantum well states (QWSs) localized in Pb overlayers on Cu(111) surface. Particular emphasis is given to the states with energies close to the vacuum level. Inclusion of the long-range image potential tail into the model potential description of the system allows us to show the effect of hybridization between QWSs and image potential states (ISs). The particle-in-a-box energy sequence characteristic for QWSs evolves into the Rydberg series converging towards the vacuum level. The electron density of the corresponding states is partially moved from inside the metal overlayer into the vacuum. The decay rates due to the inelastic electron-electron scattering decrease with increasing energy, opposite to “conventional” QWSs and similar to the ISs. Many-body and wave packet propagation calculations of the inelastic decay rates are supplemented by simple analysis based on the phase accumulation model and wave-function penetration approximation. This allows an analytical description of the dependence of the QWS/ISs hybridization on different parameters and, in particular, on the overlayer thickness.
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Procédures de Conférences |
Oughaddou H., & Kara, A. (2012). First European Mediterranean Conference on Materials & Renewable Energies (Vol. 1). Simplex Academic Publishers.
Résumé: Proceedings of the First European Mediterranean Conference on Materials & Renewable Energies (EMCMRE-1), Marrakech, Morocco, 21-25 Novembre 2011
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Actes de Conférences |
Béroff K., Nguyen-Thi V.O., Chabot M., Pino T., Tuna T., Martinet G., LePadellec A., & Do Thi N. (2012). FRAGMENTATION OF MULTIPLY-CHARGED SMALL HYDROCARBONS MOLECULES CnHq+ (n=1-3, q=2-6) PRODUCED IN HIGH VELOCITY COLLISIONS: BRANCHING RATIOS AND ASSOCIATED KINETIC ENERGY RELEASE OF THE H+ FRAGMENT. In JOURNAL OF PHYSICS-CONFERENCE SERIES (Vol. 388, 102062).
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Billaud, P., Picard, Y. J., Geleoc, M., Hergott, J. - F., Carre, B., Breger, P., Ruchon, T., Veyrinas, K., Roulliay, M., Delmotte, F., Boettcher, M., Huetz, A., & Dowek, D. (2012). Ultrafast Electronic And Nuclear Dynamics In Dissociative Photoionization Of Molecular Hydrogen and Deuterium. In XXVII INTERNATIONAL CONFERENCE ON PHOTONIC (Vol. 388).
Résumé: Single-photon dissociative photoionization of H-2/D-2 in the Q(1), Q(2) doubly excited states resonance regions, where ultrafast electronic and nuclear dynamics are coupled, is studied using the vector-correlation method with single selected femtosecond high-order harmonic and synchrotron radiation in the VUV. Results are compared at the level of electron-ion kinetic energy correlation diagrams, asymmetry parameters, and the molecular frame photoelectron angular distributions.
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Bizau, J. M., Cubaynes, D., Al Shorman, M. M., Guilbaud, S., Blancard, C., Lemaire, J., Thissen, R., Giuliani, A., Nicolas, C., & Milosavljevic, A. R. (2012). Photoionization of atomic and molecular positively charged ions. In 26TH SUMMER SCHOOL AND INTERNATIONAL SYMPOSIUM ON THE PHYSICS OF IONIZED GASES (SPIG 2012) (Vol. 399).
Résumé: We compare advantages and drawbacks of the two techniques mainly used for the experimental study of gas phase photoionization processes on ionic targets in combination with synchrotron radiation, the merged beam and ion trap. The comparison will be illustrated by recent results obtained on atomic and small molecular positively charged ions using both techniques at SOLEIL, the French synchrotron radiation facility.
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Chabot M., Béroff K., Pino T., Féraud G., Do Thi N., LePadellec A., Martinet G., Bouneau S., & Carpentier Y. (2012). NEGATIVE ION PRODUCTIONS IN HIGH VELOCITY COLLISIONS BETWEEN SMALL CARBON CLUSTERS AND HELIUM ATOME TARGET. In JOURNAL OF PHYSICS-CONFERENCE SERIES (Vol. 388, 102036).
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Gharaibeh, M. F., Bizau, J. - M., Cubaynes, D., Guilbaud, S., El Hassan, N., Al Shorman, M. M., Blancard, C., & McLaughlin, B. M. (2012). K-Shell Photoionization of Singly Ionized Atomic Nitrogen. In XXVII ICPEAC Journal of Physics: Conference Series (Vol. 388).
Résumé: K-shell photoionization cross-section measurements for singly ionized atomic nitrogen made at the SOLEIL Light Source for the first time are compared with MCDF and R-matrix calculations.
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Ideguchi, T., Bernhardt, B., Guelachvili, G., Haensch, T. W., & Picque, N. (2012). Femtosecond stimulated Raman Dual-Comb Spectroscopy. In 2012 CONFERENCE ON LASERS AND ELECTRO-OPTICS (CLEO).
Résumé: Nonlinear dual-frequency-comb spectroscopy is demonstrated with multi-heterodyne femtosecond Raman-induced Kerr-effect spectroscopy. Spectra of liquid samples are recorded with a spectral resolution of 200 GHz, a measurement time of 350 μs and a sensitivity of 10(-6).
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Ideguchi, T., Poisson, A., Guelachvili, G., Haensch, T. W., & Picque, N. (2012). Real-time Dual-comb Spectroscopy of Iodine in the Visible. In 2012 CONFERENCE ON LASERS AND ELECTRO-OPTICS (CLEO).
Résumé: Dual-comb spectroscopy is extended to the visible range. The dense rovibronic spectrum of iodine around 520 nm is measured within 12 ms at Doppler-limited resolution with a scheme that only uses free-running lasers.
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Klisnick, A. (2012). Plasma-based XUV lasers. In SHORT-WAVELENGTH IMAGING AND SPECTROSCOPY SOURCES (SPIE-INT SOC OPTICAL ENGINEERING ed., Vol. 8678, 867803). Proceedings of SPIE, 8678.
Résumé: This lecture is an introduction to the generation of plasma-based XUV lasers and their use as a source for scientific applications. We first discuss the main conditions required to create population inversions and amplify XUV radiation. We give an overview of the main properties of the different types of XUV lasers beams that are currently operational worldwide, while comparing them to other ultrashort, high-brightness sources existing in the same spectral range. We discuss recent demonstrations of applications of plasma-based XUV lasers to high-resolution imaging and interaction with matter at high intensity. Finally we conclude with current prospects for extending these sources to shorter wavelength and higher output intensity.
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Poisson, A., Ideguchi, T., Guelachvili, G., Picque, N., & Haensch, T. W. (2012). Adaptive Dual-comb Spectroscopy with Free-running Lasers and Resolved Comb Lines. In 2012 CONFERENCE ON LASERS AND ELECTRO-OPTICS (CLEO).
Résumé: A new scheme of real-time dual-comb spectroscopy that only uses free-running femtosecond lasers provides distortion-free Fourier spectra with resolved comb lines across the full spectral span of erbium-doped fiber lasers (>80 nm centered around 1550 nm) without a posteriori data processing.
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Porcel, E., Li, S., Usami, N., Remita, H., Furusawa, Y., Kobayashi, K., Le Sech, C., & Lacombe, S. (2012). Nano-Sensitization under gamma rays and fast ion radiation. In 1ST NANO-IBCT CONFERENCE 2011 – RADIATION DAMAGE OF BIOMOLECULAR SYSTEMS: NANOSCALE INSIGHTS INTO ION BEAM CANCER THERAPY (Vol. 373).
Résumé: The use of heavy compounds to enhance radiation induced damage is a promising approach to improve the therapeutic index of radiotherapy. In order to quantify and control the effects of these radiosensitizers, it is of fundamental interest to describe the elementary processes which take place at the molecular level. Using DNA as a probe, we present a comparison of the damage induced in the presence of platinum compounds exposed to different types of ionizing radiation. We present the results obtained with gamma rays (Linear Energy Transfer (LET) = 0.2 keV.mu m(-1)), fast helium ions He2+ (LET = 2.3 keV.mu m(-1)) and fast carbon ions C6+ (LET = 13 keV.mu m(-1) and LET=110 keV.mu m(-1)). The efficiency of two different sensitizers was measured: platinum based molecules (the chloroterpyridine platinum – PtTC) and platinum nanoparticles (PtNP). These experiments show that the two sensitizers are efficiently amplifying molecular damage under photon or ion irradiation. Experiments with a radical scavenger confirmed that these damages are mediated by free radicals for more than 90%. More interestingly, the induction of complex damage, the most lethal for the cells, is amplified by a factor of 1.5 on average if platinum (PtTC and PtNP) is present. As already known, the induction of complex damages increases also with the radiation LET. So, finally, the most significant enhancement of complex damage is observed when ion radiation is combined with platinum induced sensitization.
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Quirico, E., Orthous-Daunay, F. - R., Bonal, L., & et al. (2012). THE MULTIPLE ORIGINS OF THE UNSOLUBLE ORGANIC MATTER FROM PRIMITRIVE CHONDRITES. In Meteoritics & Planetary Science (Vol. 47, A323).
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Richardson, V., Costello, J. T., Nikolopoulos, L. A. A., Duesterer, S., Cubaynes, D., Meyer, M., & Li, W. B. (2012). Above-threshold two-colour ionization signal of singly charged neon. In XXVII ICPEAC Journal of Physics: Conference Series (Vol. 388).
Résumé: In this work we report the ionization of a gaseous neon target by combining extreme ultraviolet (XUV) radiation from the Free Electron Laser in Hamburg with an intense synchronized optical laser. The photoelectron spectrum dependence of the electrons ejected from singly-charged neon (Ne+) on the relative polarisation of the XUV and optical laser fields was investigated both experimentally and theoretically.
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Wang, C. Y., Herr, T., Del'Haye, P., Schliesser, A., Holzwarth, R., Haensch, T. W., Picque, N., & Kippenberg, T. J. (2012). Generation of Low Phase-noise Mid-Infrared Optical Frequency Combs from Crystalline Microresonators. In 2012 CONFERENCE ON LASERS AND ELECTRO-OPTICS (CLEO).
Résumé: We present mid-infrared frequency comb generation from crystalline MgF2 microresonators, with mode spacing of 50-150 GHz around the 2.5 μm-wavelength CW-pump. Low phase-noise is verified by beating the comb modes with a narrow line width CW laser.
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Chapitres de Livres |
Vladimir A.Esaulov. (2012). Low Energy Ion Scattering and Recoiling Spectroscopy in Surface Science. (Vol. 51, pp. 423–460). Springer Series in Surface Science. Springer-Verlag.
Résumé: This chapter presents an overview of low energy ion scattering spectroscopy and time of flight scattering and recoiling spectroscopy for the study of the structure and composition of surfaces as well as of fundamental ion surface interaction processes. The emphasis is on basic concepts regarding scattering, energy losses and charge transfer phenomena and experimental aspects involved in measurements of ion energies and time of flight measurements of scattered atoms. Some examples are provided to illustrate the type of information that can be obtained.
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