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Publications déposées dans HAL depuis 2013

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References

Articles:
•	Yang, Z., Krieger, K., Lunt, T., Brochard, F., Briançon, J-L., Neu, R., Dux, R., Janzer, A., Potzel, S., Pütterich, T. and Asdex Upgrade Team, The 3D Trajectories Construction of Controlled Tungsten Melting Droplet in ASDEX Upgrade Journal of Nuclear Materials, 438:S846-S851 2013 DOI: http://dx.doi.org/10.1016/j.jnucmat.2013.01.183 Equipe: Département CP2S : Expériences et Simulations des Plasmas Réactifs - Interaction plasma-surface et Traitement des Surfaces ESPRITS
•	Hicks, J., Tejeda, A., Taleb-Ibrahimi, A., Nevius, M. S., Wang, F., Shepperd, K., Palmer, J., Bertran, F., Le Fèvre, P., Kunc, J., de Heer, W. A., Berger, C. and Conrad, E. H. A wide-bandgap metal-semiconductor-metal nanostructure made entirely from graphene NATURE PHYSICS, 9(1):49-54 2013 ISSN: 1745-2473 DOI: 10.1038/NPHYS2487 Equipe: Département P2M : Surfaces et Spectroscopies
•	Kalitsov, A., Zermatten, P.-J., Bonell, F., Gaudin, G., Andrieu, S., Tiusan, C., Chshiev, M. and Velev, J.P. Bias dependence of tunneling magnetoresistance in magnetic tunnel junctions with asymmetric barriers Journal of Physics Condensed Matter, 25(49) 2013 http://www.scopus.com/inw...41c1f5d830deccd7e86a3e979 Equipe: Département P2M : Nanomagnétisme et Electronique de Spin
•	Cortes, R., Tejeda, A., Lobo-Checa, J., Didiot, C., Kierren, B., Malterre, D., Merino, J., Flores, F., Michel, E. G. and Mascaraque, A. Competing charge ordering and Mott phases in a correlated Sn/Ge(111) two-dimensional triangular lattice PHYSICAL REVIEW B, 88(12) 2013 ISSN: 1098-0121 DOI: 10.1103/PhysRevB.88.125113 Equipe: Département P2M : Surfaces et Spectroscopies
•	Hamdan, A., Noel, C., Kosior, F., Henrion, G. and Belmonte., T. Dynamics of bubbles created by plasma in heptane for micro-gap conditions Journal of the Acoustical Society fo America, 134:991 2013 DOI: http://dx.doi.org/10.1121/1.4812255 Resume: The determination of the initial pressure at the bubble wall created by a discharge in heptane for micro-gap conditions cannot be determined straightforwardly by modeling the time-oscillations of the bubble. The resolution of the Gilmore equation gives the same solutions beyond 1 mu s typically for various sets of initial parameters, making impossible the determination of the initial pressure at the bubble wall. Furthermore, the very first instant of the bubble formation is not easily accessible at very short time scales because of the plasma emission. Since the pressure waves propagate in the liquid, it is much easier to gain information on the first instants of the bubble formation by studying the pressure field far from the emission source. Then, it is possible to deduce by modeling what happened at the beginning of the emission of the pressure waves. The proposed solution consists in looking at the oscillations affecting another bubble located at least twice farther from the interelectrode gap than the maximum radius reached by the discharge bubble. The initial plasma pressure can be determined by this method. (C) 2013 Acoustical Society of America. Equipe: Département CP2S : Expériences et Simulations des Plasmas Réactifs - Interaction plasma-surface et Traitement des Surfaces ESPRITS
•	Hamdan, A., Noel, C., Kosior, F., Henrion, G. and Belmonte, T. Dynamics of bubbles created by plasma in heptane for micro-gap conditions JOURNAL OF THE ACOUSTICAL SOCIETY OF AMERICA, 134(2, 1):991-1000 Belmonte, T (Reprint Author), Univ Lorraine, Inst Jean Lamour, UMR CNRS 7198, Parc Saurupt,CS 14234, F-54042 Nancy, France. Hamdan, A.; Noel, C.; Kosior, F.; Henrion, G.; Belmonte, T., Univ Lorraine, Inst Jean Lamour, UMR CNRS 7198, F-54042 Nancy, France. 2013 ISSN: 0001-4966 DOI: 10.1121/1.4812255 Resume: The determination of the initial pressure at the bubble wall created by a discharge in heptane for micro-gap conditions cannot be determined straightforwardly by modeling the time-oscillations of the bubble. The resolution of the Gilmore equation gives the same solutions beyond 1 mu s typically for various sets of initial parameters, making impossible the determination of the initial pressure at the bubble wall. Furthermore, the very first instant of the bubble formation is not easily accessible at very short time scales because of the plasma emission. Since the pressure waves propagate in the liquid, it is much easier to gain information on the first instants of the bubble formation by studying the pressure field far from the emission source. Then, it is possible to deduce by modeling what happened at the beginning of the emission of the pressure waves. The proposed solution consists in looking at the oscillations affecting another bubble located at least twice farther from the interelectrode gap than the maximum radius reached by the discharge bubble. The initial plasma pressure can be determined by this method. (C) 2013 Acoustical Society of America. Equipe: Centre de Compétences : ERMIONE informatique et calcul
•	Margueron, Samuel, Bartasyte, Ausrine, Plausinaitiene, Valentina, Abrutis, Adulfas, Boulet, Pascal, Kubilius, Virgaudas and Saltyte, Zita Effect of deposition conditions on the stoichiometry and structural properties of LiNbO3 thin films deposited by MOCVD 8626 2013 ISSN: 0277-786X DOI: 10.1117/12.2010105 Equipe: Centre de Compétences : X-Gamma rayons X et spectroscopie
•	Vasseur, Guillaume, Fagot-Revurat, Yannick, Kierren, Bertrand, Sicot, Muriel and Malterre, Daniel Effect of Symmetry Breaking on Electronic Band Structure: Gap Opening at the High Symmetry Points SYMMETRY-BASEL, 5(4):344-354 2013 ISSN: 2073-8994 DOI: 10.3390/sym5040344 Equipe: Département P2M : Surfaces et Spectroscopies
•	Zhang, H.Y., Cleymand, F., Noel, C., Kahn, C.J.F., Linder, M., Dahoun, A., Henrion, G. and Arab-Tehrany, E. Effects of Ar-H2-N2 microwave plasma on chitosan 1 and its nanoliposomes blend thin films designed for tissue engineering applications Carbohydrate Polymers, 93(2):401-411 2013 DOI: http://dx.doi.org/10.1016/j.carbpol.2012.12.015 Resume: This work addresses the functionalization of chitosan thin films and its nanoliposomes blend films by a microwave-excited Ar/N2/H2 surface-wave plasma treatment which was found an effective tool to modify surface properties. Changes in the film properties (wettability, chemical composition, morphology) induced by the plasma treatment are studied using water contact angle measurements, X-ray photoelectron spectroscopy and scanning probe microscopy. The results suggest that hydrophilicity of the films is improved by plasma treatment in a plasma condition dependency manner. Water contact angle of chitosan films before and after plasma treatment are, respectively, 101Â° and 27Â°. Besides chemical changes on the surface, the nanoliposomes incorporation and plasma treatment also induce morphological modifications. Moreover, a correlation is found between the nanoliposomes composition and size, and the effects of plasma treatment. It is shown that the plasma treatment significantly improves the chitosan film functionalization. The effect of N2 content (88% and 100%) in the plasma gas mixture on the film etching is also pointed out. Equipe: Département CP2S : Expériences et Simulations des Plasmas Réactifs - Interaction plasma-surface et Traitement des Surfaces ESPRITS
•	Tournier-Colletta, C., Kierren, B., Fagot-Revurat, Y. and Malterre, D. Electron hopping at the Si(111):B-root 3 surface: Insight from local impurity spectroscopy PHYSICAL REVIEW B, 87(7) 2013 ISSN: 1098-0121 DOI: 10.1103/PhysRevB.87.075427 Equipe: Département P2M : Surfaces et Spectroscopies

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