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References

Articles:
2014
•	Hauet, T., Piraux, L., Srivastava, S.K., Antohe, V.A., Lacour, D., Hehn, M., Montaigne, F., Schwenk, J., Marioni, M.A., Hug, H.J., Hovorka, O., Berger, A., Mangin, S. and Abreu Araujo, F. Reversal mechanism, switching field distribution, and dipolar frustrations in Co/Pt bit pattern media based on auto-assembled anodic alumina hexagonal nanobump arrays Physical Review B - Condensed Matter and Materials Physics, 89(17) 2014 http://www.scopus.com/inw...59f73e3cc90d9e16f1ec3fa21 Equipe: Département P2M : Nanomagnétisme et Electronique de Spin
•	Exbrayat, L., Calvié, E., Douillard, T., Marcos, G., Savall, C., Berziou, C., Creus, J. and Steyer, P. Role of ceria nanoparticles on the electrodeposition zinc coatingâ??s growthÂ : Interest of a TEM-Scale investigation ECS Electrochemistry Letters, 39:D33-D35 2014 DOI: 10.1149/2.0011410eel Equipe: Département CP2S : Expériences et Simulations des Plasmas Réactifs - Interaction plasma-surface et Traitement des Surfaces ESPRITS
•	Shin, Heekeun, Schwarze, A., DIEHL, R. D., PUSSI, K., Colombier, A., Gaudry, E., Ledieu, J., McGuirk, G. M., Loli, L. N. Serkovic, Fournee, V., Wang, L. L., Schull, G. and Berndt, R. Structure and dynamics of C-60 molecules on Au(111) PHYSICAL REVIEW B, 89(24) 2014 ISSN: 1098-0121 DOI: 10.1103/PhysRevB.89.245428 Equipe: Département CP2S : Métallurgie et Surfaces
•	Cui, C., Nugent, P. J., Shimoda, M., Ledieu, J., Fournee, V., Tsai, A. P., McGrath, R. and SHARMA, H. R. Structure of the twofold surface of the icosahedral Ag-In-Yb quasicrystal JOURNAL OF PHYSICS-CONDENSED MATTER, 26(1) 2014 ISSN: 0953-8984 DOI: 10.1088/0953-8984/26/1/015001 Equipe: Département CP2S : Métallurgie et Surfaces
•	Alebrand, S., Bierbrauer, U., Hehn, M., Gottwald, M., Schmitt, O., Steil, D., Fullerton, E.E., Mangin, S., Cinchetti, M. and Aeschlimann, M. Subpicosecond magnetization dynamics in TbCo alloys Physical Review B - Condensed Matter and Materials Physics, 89(14) 2014 http://www.scopus.com/inw...4c6d76c54882c79454e3c7176 Equipe: Département P2M : Nanomagnétisme et Electronique de Spin
•	Badinier, G., Sinclair, C.W., Allain, S. and Bouaziz, O. The Bauschinger effect in drawn and annealed nanocomposite Cu--Nb wires Materials Science & Engineering A, 597:10-19 2014 DOI: http://dx.doi.org/10.1016/j.msea.2013.12.03 Equipe: Département SI2M : Microstructures et Contraintes
•	Bergeard, N., López-Flores, V., Halté, V., Hehn, M., Stamm, C., Pontius, N., Beaurepaire, E. and Boeglin, C. Ultrafast angular momentum transfer in multisublattice ferrimagnets Nature Communications, 5 2014 http://www.scopus.com/inw...64357aa837533ddbda962f1c8 Equipe: Département P2M : Nanomagnétisme et Electronique de Spin
2013
Articles:
•	Gazeli, K., Noel, C., Clement, F., Daugé, C., Svarnas, P. and Belmonte, T. A study of helium atmospheric-pressure guided streamers for potential biological applications Plasma Sources Science and Technology, 22:025020 2013 DOI: http://dx.doi.org/10.1088/0963-0252/22/2/025020 Resume: The origin of differences in the rotational temperatures of various molecules and ions (N-2(+)(B), OH(A) and N-2(C)) is studied in helium atmospheric-pressure guided streamers. The rotational temperature of N-2(+)(B) is room temperature. It is estimated from the emission band of the first negative system at 391.4 nm, and it is governed by the temperature of N-2(X) in the surrounding air. N-2(X) is ionized by direct electron impact in the outer part of the plasma. N-2(+)(B) is deactivated by collisions with N-2 and O-2. The rotational temperature of OH(A), estimated from the OH band at 306.4 nm, is slightly higher than that of N-2(+)(B). OH(A) is excited by electron impact with H2O during the first 100 ns of the applied voltage pulse. Next, OH(A) is produced by electron impact with OH(X) created by the quenching of OH(A) by N-2 and O-2. H2O diffuses deeper than N-2 into the plasma ring and the rotational temperature of OH(A) is slightly higher than that of N-2(+)(B). The rotational temperature of N-2(C), estimated from the emission of the second positive system at 315.9 nm, is governed by its collisions with helium. The gas temperature of helium at the beginning of the pulse is predicted to be several hundred kelvin higher than room temperature. 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
•	Pushkareva, I., Scott, C., Goune, M., Valle, N., Redjaïmia, A. and Moulin, A Distribution of Carbon in Martensite During Quenching and Tempering of Dual Phase Steels and Consequences for Damage Properties. ISIJ International, 53:1215-1223 2013 DOI: 10.2355/isijinternational.53.1215 Equipe: Département SI2M : Microstructures et Contraintes

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