This file was created by the Typo3 extension sevenpack version 0.7.16 --- Timezone: CEST Creation date: 2019-10-19 Creation time: 07-11-01 --- Number of references 29 article 201-4447 Analytical Chemistry 2014 86 11217-11225 Département CP2S : ESPRITS 10.1021/ac502774m C.Turgut G.Sinha L.Mether J.Lahtinen K.Nordlund M.Belmahi P.Philipp article 201-4445 Applied Physics Letters 2014 105 181120-181124 Département CP2S : ESPRITS 10.1063/1.4901440 M.Desecures L.de Poucques T.Easwarakhanthan J.Bougdira article 201-4430 Journal of Alloys and Compounds 2014 587 303-307 Département CP2S : ESPRITS 10.1016/j.jallcom.2013.10.100 O.Meglali N.Attaf A.Bouraiou J.Bougdira M.S.Aida article 201-4354 Plasma Chemistry and Plasma Processing 2014 34 1101-1114 Département CP2S : ESPRITS 10.1007/s11090-014-9564-y A.Hamdan C.Noel J.Ghanbaja T.Belmonte article 201-4341 Nuclear Instruments and Methods in Physics Research B: Beam Interactions with Materials and Atoms 2014 326 341-344 The deposition of multiple carbon atoms on a crystalline silicon (Si) surface is modelled at 5 eV energy by using molecular dynamics simulations combined with a third generation force field that includes bond breaking and formation. Force field parameters are taken from a previous work. These simulations allow for atomic scale insights into the deposition mechanisms and an easier comparison with experimental observations. The results, including distributions of implantation depth, carbon concentrations, sticking coefficients, radial distribution function, and angular distributions are compared for different incidence angles. Due to the deposition of carbon atoms inside the silicon structure, silicon carbide starts to form. The crystalline structure has been investigated for different conditions to get a better understanding of the damaging and growth mechanisms. It is found that a lot of deformation is accumulated in the area of deposition near to the surface but underneath the surface the silicon has still a more crystalline structure. The variation of the silicon (carbide) structu re slightly depends on the angle of incidence. For the conditions used for these simulations, the sticking probability is always high and varies between 95% and 100%, which can be attributed to the high affinity of carbon for silicon. Département CP2S : ESPRITS 10.1016/j.nimb.2013.10.069 A.Jana L.Briquet T.WIRTZ P.Philipp G.Henrion article 201-4355 Journal of Crystal Growth 2014 407 17-24 Département CP2S : ESPRITS 10.1016/j.jcrysgro.2014.08.029 A.Altaweel G.Filipic T.Gries T.Belmonte article 201-4352 Oxidation of Metals 2014 82 163-179 Département CP2S : ESPRITS 10.1007/s11085-014-9484-5 E.K. Tillous J.Dulcy T.Belmonte article 201-4431 Materials Science in Semiconductor Processing 2014 17 38-42 Département CP2S : ESPRITS 10.1016/j.mssp.2013.08.004 M.Messaoudi M.S. Aida N.Attaf T.Bezzi J.Bougdira G.Medjahdi article 201-4342 Journal of Physics D: Applied Physics 2014 47 205201 The electron temperature and electron density are measured in a microwave (MW) plasma-assisted chemical vapour diamond deposition reactor for different experimental conditions by varying the substrate temperature, methane content and MW power density. Optical emission spectroscopy (OES) and MW interferometry are used to probe the discharge generated in a stainless steel resonant cavity excited at a frequency of 2.45 GHz. Changing the substrate temperature from 630 to 900 ◦C does not show any significant influence on the electron temperature or on the electron density. Increasing the methane content from 0 to 10% does not lead to any modification of the electron temperature or density. However between 10% and 20% CH, a decrease of the electron density is observed which may be attributed to soot particle formation. The electron density increases in the range of (1.2–10) × 1011 cm−3 from moderate power density conditions (50 hPa/1000 W) to high power density conditions (250 hPa/3500 W). OES measurements show that the electron temperature exhibits a flat axial profile in the plasma bulk and ranges from 14 000K at (25 hPa/600 W) to 10 500K at (400 hPa/3000 W). Département CP2S : ESPRITS 10.1088/0022-3727/47/20/205201 N.Derkaoui C.Rond T.Gries G.Henrion A.Gicquel article 201-4429 Physica Scripta 2014 2014 T161 014052 Département CP2S : ESPRITS 10.1088/0031-8949/2014/T161/014052 MoradEl Kaouini HassanChatei JamalBougdira article 201-4351 Materials Chemistry and Physics 2014 147 623-628 Département CP2S : ESPRITS 10.1016/j.matchemphys.2014.05.040 S.Margueron S.Ropers F.Genty A.Bartasyte T.Belmonte article 201-4446 Surface and Interface Analysis 2014 46 357-359 Département CP2S : ESPRITS 10.1002/sia.5649 C.Turgut T.WIRTZ M.Belmahi P.Philipp article 201-4357 Plasma Processes and Polymers 2014 in press Silicon nanostructures are synthesized with a DC atmospheric pressure microplasma jet using an Ar/SiH4/H2 gas mixture. The plasma is characterized by OES and imaged using an EMCCD camera. The effect of hydrogen admixture to the formed structures is studied by transmission electron microscopy. Under specific conditions, crystalline silicon nanoparticles grow in an amorphous matrix investigated by electron energy loss spectroscopy. As-grown silicon nanoparticles are collected in ethanol for dynamic light scattering and photoluminescence measurements. The size distribution peaks at 4 nm. The silicon nanocrystals exhibit roomtemperature photoluminescence that peaks at ~415 and ~465 nm Département CP2S : ESPRITS 10.1002/ppap.201400047 B.Barwe A.Stein O.E. Cibulka J.Ghanbaja T.Belmonte J.Benedikt article 201-4348 Surface and Coatings Technology 2014 255 3-7 Département CP2S : ESPRITS 10.1016/j.surfcoat.2013.10.040 D.Kuete Saa R.P.Cardoso F.Kosior A.Altaweel T.Gries S.Laminsi T.Belmonte article 201-4176 Surface and Coatings Technology 2014 In Press - available on line The chemical stability of the electrolyte in Plasma Electrolytic Oxidation (PEO) has been the subject of much systematic investigation. The present study reports on experimental results on the ageing of a usual PEO electrolyte and its effect on the oxidation of the Al2214 aluminium alloy. A solution of potassium hydroxide ([KOH] = 1 g/L) and sodium silicate ([Na2SiO3] = 1.65 g/L) diluted in deionized water was either aged by running a process during 8 h at most or not. Comparison between materials treated in either solution was made next. Cross-checked experimental results from analytical chemistry, plasma diagnostics and materials science clearly evidence the effect of ageing of the electrolyte on the PEO process behaviour. The transition from arc to "soft" regime occurs earlier (from 18 min to 13 min processing time) as the electrolyte gets older. The concomitant decrease in the electrolyte electrical conductivity (from 7.5 mS.cm-1 to 6.8 mS.cm-1) is correlated with changes in the ionic species content in the electrolyte. Fast video-imaging (125 kfr./s) reveals that the micro-discharge characteristics are also sensitive since they become less numerous per area and unit time (from 220.103 cm-2s-1 to 120.103 cm-2s-1), exhibit shorter lifetime and have smaller sizes as the electrolyte ages. SEM observations of the as-grown coatings combined with roughness measures indicate a decrease in coating thickness ( ~ 20 %) and roughness ( ~ 30 %) while species from the electrolyte accumulate in the outer porous layer simultaneously with a gradual enrichment in a-Al2O3 phase in the inner compact layer (from 36 % to 43 %). Finally, within the PEO conditions that were used, it is shown that the ageing phenomenon of the PEO electrolyte starts to influence the process after 2 hours aged. Département CP2S : ESPRITS 10.1016/j.surfcoat.2014.11.001 J.Martin P.Leone A.Nominé D.Veys-Renaux G.Henrion T.Belmonte article 201-4179 Electrochimica Acta 2014 124 30-45 In the framework of the new ecological regulations, micro-arc oxidation (MAO) appears as an alternativeto usual processes in the field of corrosion protection of Mg alloys. In this work, the initial stagesof anodic layer growth in KOH-based electrolytes are studied up to and beyond the initiation of themicro-arc regime.The properties of the first anodized film preceding the occurrence of the dielectric breakdown (corre-sponding to the start of the micro-arc regime) are mainly determined by the incorporation of additives(fluorides or silicates) in the film, as shown by in situ electrochemical measurements. Scanning electronmicroscopy (SEM), X-ray photoelectron spectroscopy (XPS) and micro-Raman spectroscopy reveal boththe change of morphology and chemical state of silicate and fluoride in the anodized layer before andafter the micro-arc regime. In terms of electrochemical behaviour, investigated by stationary methodsand electrochemical impedance spectroscopy (EIS) in reference corrosive water, the anodic film grownin the silicate medium provides the best corrosion resistance thanks to a thick layer containing Mg2SiO4,whose degradation products seal the porosities of the coating. Département CP2S : ESPRITS 10.1016/j.electacta.2013.08.023 D.Veys-Renaux E.ROCCA J.Martin G.Henrion article 201-3917 Journal of Physics D: Applied Physics 2014 47 224016 (18 pp) Discharge–surface interaction in liquids includes many phenomena which are reviewed in this work. This is used to examine results in the area of nanoparticle synthesis and to propose a general sketch of formation mechanisms. Département CP2S : ESPRITS 10.1088/0022-3727/47/22/224016 T.Belmonte A.Hamdan F.Kosior C.Noel G.Henrion article 201-4413 ACS Applied Materials and Interfaces 2014 6 13707-13715 Département CP2S : ESPRITS 10.1021/am503160w T.Gries R.Catrin S.Migot F.SOLDERA J.L.Endrino A.R.Landa-Cánovas F.Cleymand D.Mangin F.Mücklich D.Horwat article 201-4347 Images in Plasma Science 2014 99 1 Département CP2S : ESPRITS 10.1109/TPS.2014.2308402 A.Hamdan I.Marinov A.Rousseau T.Belmonte article 201-4381 Surface and Coatings Technology 2014 259 737-745 Département CP2S : ESPRITS 10.1016/j.surfcoat.2014.09.065 Y.Samih G.Marcos N.Stein N.Allain E.Fleury C.Dong T.Grosdidier article 201-4349 Journal of Physics D: Applied Physics 2014 47 265201 Département CP2S : ESPRITS 10.1088/0022-3727/47/26/265201 M.Santos C.Noel T.Belmonte L.L. Alves article 201-4443 Plasma Processes and Polymers 2014 11 551-558 Département CP2S : ESPRITS 10.1002/ppap.201300166 M.Belmahi S.Bulou A.Thouvenin L.de Poucques R.Hugon L.Le Brizoual P.Miska D.Genève J.-L.Vasseur J.Bougdira article 201-3916 Surface and Coatings Technology 2014 238 27-44 The kinetic aspects of the coating formation on the 2024 aluminium alloy at different time intervals of the microarc oxidation process(MAO) in an alkaline–silicate electrolyte under the AC current are investigated.Moreover themain reasons of modifications in theMAO coating properties (corrosion resistance,microhardness) and phase composition during the process are shown. Finally, non-destructive controlmethods ofMAO coating properties are worked out. Département CP2S : ESPRITS 10.1016/j.surfcoat.2013.10.032 I.Shchedrina A.G.Rakoch G.Henrion J.Martin article 201-4350 Applied Surface Science 2014 311 721-728 Département CP2S : ESPRITS 10.1016/j.apsusc.2014.05.145 N.D. Boscher S.Olivier R.Maurau S.Bulou T.Sindzingre T.Belmonte P.Choquet article 201-4444 Carbon 2014 76 330-340 Département CP2S : ESPRITS 10.1016/j.carbon.2014.04.084 X.Glad L.de Poucques J.A. Jaszczak M.Belmahi J.Ghanbaja J.Bougdira article 201-4380 ECS Electrochemistry Letters 2014 39 D33-D35 Département CP2S : ESPRITS 10.1149/2.0011410eel L.Exbrayat E.Calvié T.Douillard G.Marcos C.Savall C.Berziou J.Creus P.Steyer article 201-4353 Materials Letters 2014 135 115–118 Département CP2S : ESPRITS 10.1016/j.matlet.2014.07.158 A.Hamdan C.Noel T.Belmonte article 201-4177 Applied Physics Letters 2014 104 081603 Plasma electrolytic oxidation (PEO) processing of EV31 magnesium alloy has been carried out in fluoride containing electrolyte under bipolar pulse current regime. Unusual PEO cathodic microdischarges have been observed and investigated. It is shown that the cathodic micro-discharges exhibit a collective intermittent behavior, which is discussed in terms of charge accumulations at the layer/electrolyte and layer/metal interfaces. Optical emission spectroscopy is used to determine the electron density (typ. 1015cm_3) and the electron temperature (typ. 7500K) while the role of F_ anions on the appearance of cathodic micro-discharges is pointed out. Département CP2S : ESPRITS 10.1063/1.4866425 A.Nominé J.Martin C.Noel I.V. Bardin V.L. Kovalev T.Belmonte A.G. Rakoch G.Henrion article 201-4346 Journal of Physics D: Applied Physics 2014 47 055203 Département CP2S : ESPRITS 10.1088/0022-3727/47/5/055203 A.Hamdan I.Marinov A.Rousseau T.Belmonte