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References

2014

Articles:

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.
Physical Review B - Condensed Matter and Materials Physics, 89(17)
2014

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.
ECS Electrochemistry Letters, 39:D33-D35
2014

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.
PHYSICAL REVIEW B, 89(24)
2014
ISSN: 1098-0121

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.
JOURNAL OF PHYSICS-CONDENSED MATTER, 26(1)
2014
ISSN: 0953-8984

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.
Physical Review B - Condensed Matter and Materials Physics, 89(14)
2014

Equipe: Département P2M : Nanomagnétisme et Electronique de Spin

Badinier, G., Sinclair, C.W., Allain, S. and Bouaziz, O.
Materials Science & Engineering A, 597:10-19
2014

Equipe: Département SI2M : Microstructures et Contraintes

Bergeard, N., López-Flores, V., Halté, V., Hehn, M., Stamm, C., Pontius, N., Beaurepaire, E. and Boeglin, C.
Nature Communications, 5
2014

Equipe: Département P2M : Nanomagnétisme et Electronique de Spin

2013

Articles:

Gazeli, K., Noel, C., Clement, F., Daugé, C., Svarnas, P. and Belmonte, T.
Plasma Sources Science and Technology, 22:025020
2013

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.
NATURE PHYSICS, 9(1):49-54
2013
ISSN: 1745-2473

Equipe: Département P2M : Surfaces et Spectroscopies

Pushkareva, I., Scott, C., Goune, M., Valle, N., Redjaïmia, A. and Moulin, A
ISIJ International, 53:1215-1223
2013

Equipe: Département SI2M : Microstructures et Contraintes

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