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ICMCTF 2012! - CD-Lab Application Oriented Coating Development

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Post Deadline Discoveries and Innovations<br />

Room: Pacific Salon 1-2 - Session PD-1<br />

Post Deadline Discoveries and Innovations<br />

Moderator: W. Kalss, OC Oerlikon Balzers AG,<br />

Liechtenstein, S. Ulrich, Karlsruhe Institute of Technology,<br />

Germany<br />

1:30pm PD-1-1 The Multi Beam Sputtering: a new thin film deposition<br />

approach, P. Sortais (sortais@lpsc.in2p3.fr), T. Lamy, J. Médard,<br />

<strong>Lab</strong>oratoire de Physique Subatomique et Cosmologie de Grenoble (LPSC),<br />

France<br />

Thanks to the latest development of ultra compact and reliable microwave<br />

ion sources 1,2 it is now possible to build an ion beam sputterring system<br />

composed of an arbitrary large number of simple ion sources that can be<br />

individually tuned. With this new concept of Multi Beam Sputtering (MBS)<br />

device, new possibilities are conceivable for the Ion Beam Sputtering (IBS)<br />

technology 3,4 , especially for thin film deposition on large size substrates<br />

with high uniformity. With MBS, the deposition profile is not defined by<br />

the shape and the tuning of a unique large beam, but by the sum of the<br />

contributions of a great number of small, well controlled in size, sputterring<br />

spots. The uniformity is the consequence of the geometric sum of all<br />

sputterring lobes obtained by each sputtering spot. The ion sources units can<br />

be distributed along a circle or a line and each ion beam delivered by an ion<br />

source impinges its own target. An individual source of a typical size 3x3x3<br />

cm uses a few watts of microwave power for producing a beam up to 1 mA<br />

with energy in the range of 5 to 15 keV. The first operational device, MBS-<br />

20, uses 20 of such ion sources distributed on a circle around a 70 mm<br />

diameter multi-target holder allowing thin film deposition on 100 to 300<br />

mm diameter substrates with deposition rates in the range of 0 to 1 µm/h.<br />

An important point, since each ion source uses an individual target, is that<br />

co-evaporation of several components can be done simultaneously. By the<br />

way, the deposition of alloys with a controlled stoechiometry is easier than<br />

with any other method and without uniformity loss. We will show<br />

preliminary results for Cu, Ta, Ta2O5, C, Si02, Ti, TiN, TiO2, TiAlN and Th<br />

on 100 or 200 mm glass substrate diameters, Mylar 0.5 µm or Si substrates.<br />

All these processes can be done with reactive atmosphere allowing oxide or<br />

nitride deposition.<br />

1<br />

P. Sortais, T. Lamy, J. Médard, J. Angot, L. Latrasse, and T. Thuillier, Rev.<br />

Sci. Instrum. 81 (2010) 02B31<br />

2<br />

P. Sortais, T. Lamy, J. Médard, J. Angot, P. Sudraud et al., Rev. Sci.<br />

Instrum. 83, 02B912 (<strong>2012</strong><br />

3<br />

Patent pending N° 1150981.<br />

4<br />

Under Grant Grenoble Alpes Valorisation Innovation Technologies<br />

(GRAVIT) 080606, may 2009.<br />

1:50pm PD-1-2 Molecular dynamics simulation and experimental<br />

validation of nanoindentation measurements of silicon carbide<br />

coatings., A.-P. Prskalo (alen-pilip.prskalo@imwf.uni-stuttgart.de),<br />

Universität Stuttgart, Germany, S. Ulrich, Karlsruhe Institute of<br />

Technology, Germany, S. Schmauder, J. Lichtenberg, , C. Ziebert, Kit, Iam-<br />

Awp, Germany<br />

Molecular dynamics simulation of the nanoindentation was used to<br />

investigate mechanical properties of single layer silicon carbide coatings on<br />

silicon substrates. Indenter load-penetration depth relation was determined<br />

and put into relation to the internal coating structure and the substrate<br />

behavior. In order to reach this objective, an indenter tip in the form of a<br />

Berkovich indenter was introduced, a discrete indenter motion of 0.2 Å was<br />

imposed. For the modeling of the Si-C system, well known bond-order<br />

Tersoff potential was used, while the substrate-indenter interaction was<br />

modeled by a self-developed short range repulsive pair potential. From the<br />

indenter load-penetration depth relation, mechanical values of hardness and<br />

Young modulus for the coatings could be obtained. Hardness values<br />

determined by molecular dynamics simulations were in the range between<br />

26.4 GPa and 34.4 GPa. These results are in good agreement with<br />

experimental measurements using UMIS 2000 system delivering values<br />

between 20.1 GPa and 35 GPa in dependence of the micro structure of the<br />

coating, the deposition temperature and maximum indentation depth.<br />

2:10pm PD-1-3 Anatase TiO2 Beads Having Ultra-fast Electron<br />

Diffusion Rates for use in Low Temperature Flexible Dye-sensitized<br />

Solar Cells, J.-M. Ting (jting@mail.ncku.edu.tw), Ke, National Cheng<br />

Kung University, Taiwan<br />

The first use of mesoporous TiO2 beads in plastic substrate flexible dyesensitized<br />

solar cell (FDSC) is demonstrated. Pure anatase TiO2 beads with<br />

various sizes (250 to 750 nm) and characteristics are obtained using a<br />

Thursday Afternoon, April 26, <strong>2012</strong> 92<br />

modified and efficient two-step method. The concept of chemical sintering,<br />

eliminating the step of additive removal, is used to prepare bead-containing<br />

paste for room temperature fabrication of photoanode having good adhesion<br />

to the substrate. The obtained photoanodes are examined for their dye<br />

loadings and light absorbance properties. Various plastic substrate FDSCs<br />

having commercial P25- and bead-containing photoanodes are fabricated<br />

and evaluated. The resulting cells are evaluated for the J-V characteristics,<br />

electron diffusion time, electron lifetime, charge-collection efficiency,<br />

electron-injection efficiency and incident photon-to-electron conversion<br />

efficiency. The bead-only cells not only have better efficiencies, as high as<br />

~5%, but also exhibit ultra-fast electron diffusion rates, less than 1 ms. The<br />

best efficiency and electron diffusion rates are respectively 15% higher and<br />

two-order of magnitude faster than the P25-only cell. The effects of the<br />

bead characteristics on the cell performance is presented and discussed.<br />

2:30pm PD-1-4 MOCVD nano-structured TiO2 coatings for corrosion<br />

protection of stainless steels, H. Herrera-Hernández<br />

(hhh@correo.azc.uam.mx), M. Palomar-Pardavé, Universidad Autónoma<br />

Metropolitana- Azcapotzalco, Mexico, J.A. Galaviz-Pérez, J.R. Vargas-<br />

García, Departamento de Ingeniería, Metalúrgica, ESIQIE-IPN, Mexico<br />

TiO2 nanoparticles were deposited on 316 stainless steel substrates at three<br />

different temperatures using a horizontal hot-wall reactor in the presence of<br />

a titanium isopropoxide Ti(OC3H7)4 precursor, method known as metal<br />

organic chemical vapor deposition (MOCVD). The influence of deposition<br />

temperature (Tdep 300, 400 and 500 ºC) on the structural and protective<br />

properties of the TiO2 nanoparticles was discussed. The morphology and<br />

structure of these nanoparticles that form a continuous thin coating over the<br />

steel was investigated by X-ray diffraction (XRD), energy dispersive<br />

spectroscopy (EDS) and scanning electron microscopy (SEM) techniques.<br />

The corrosion resistance of the TiO2 coatings was evaluated in a strong<br />

corrosive solution (0.5M H2SO4) by means of electrochemical<br />

measurements such as anodic polarization, cyclic voltammetry (CV) and<br />

electrochemical impedance spectroscopy (EIS). Anodic polarization results<br />

revealed that the pitting corrosion potential (Epit) shifted to a more positive<br />

when the deposition temperature increased in comparison to the bare<br />

substrate, while CV behaviour showed lower passive current density for<br />

TiO2 coatings. Through the EIS data it was found that TiO2 nanoparticles<br />

deposited at 500 ºC for 30 min did not corroded by pits during over<br />

exposure for 100 days in such aggressive electrolyte. A higher electrical<br />

coating resistance (RTiO2 = 59.52 KW-cm 2 ) and lower capacitance (CTiO2=<br />

87.37 mF/cm 2 ) was measured for 500 ºC TiO2 coating in contrast to 300 or<br />

400 ºC coatings.<br />

The improve pitting corrosion resistance for TiO2 nanoparticles deposited at<br />

500 ºC is attributed to its morphology features and its uniform & compact<br />

anatase structure, which consisted of platelets agglomerates with very small<br />

quasi-spherical nano-particles (10~nm) that impedes the free transfer of<br />

electrons and mass-transport process across the coating. Therefore, stainless<br />

steels surface modification with TiO2 nanoparticles showed excellent<br />

corrosion resistance for long times exposure in sulphuric acid that makes it<br />

an attractive material for biomedical applications.<br />

2:50pm PD-1-5 Improvement on the mechanical and corrosion<br />

properties of nanometric HfN/VN superlattices, P. Prieto, Excellence<br />

Center for Novel Materials, CENM, Cali, Colombia, C.A. Escobar,<br />

Universidad del Valle, Colombia, J.C. Caicedo, Universidad del Valle,<br />

Colombia, W. Aperador, Universidad Militar Nueva Granada, Colombia, J.<br />

Esteve, M.E. Gomez, Universitat de Barcelona, Spain<br />

The aim of this work is the improvement of the mechanical and<br />

electrochemical behavior of 4140 steel substrate using HfN/VN<br />

multilayered system as a protective coating. We have grown HfN/VN<br />

multilayered via reactive r.f. magnetron sputtering technique in which was<br />

varied systematically the bilayer period (Λ), and the bilayer number (n),<br />

maintaining constant the total thickness of the coatings (~1.2 μm). The<br />

coatings were characterized by X-ray diffraction (XRD), X-ray photo<br />

electron spectroscopy (XPS), electron microscopy assisted with selected<br />

area electron diffraction. The mechanical properties were analyzed by<br />

nanoindentation method. The electrochemical properties were studied by<br />

Electrochemical Impedance Spectroscopy and Tafel curves. XRD results<br />

showed a preferential growth in the face-centered cubic (111) crystal<br />

structure for [HfN/VN]n multilayered coatings. The best improvement of<br />

the mechanical behavior was obtained when the bilayer period (Λ) was 15<br />

nm (n = 80), yielding the highest hardness (37 GPa) and elastic modulus<br />

(351 GPa). The values for the hardness and elastic modulus are 1.48 and<br />

1.32 times greater than the coating with n = 1, respectively. The<br />

enhancement effects in multilayer coatings could be attributed to different<br />

mechanisms for layer formation with nanometric thickness due to the Hall-<br />

Petch effect. The maximum corrosion resistance was obtained for coating<br />

with (Λ) equal to 15 nm, corresponding to n = 80 bilayered. The<br />

polarization resistance and corrosion rate were around 112.19 kOhm cm 2<br />

and 3.66x10 -3 mm/year, these values were 98 % and 99 % better than those

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