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H multilayer coatings development with a built-in mechanism of controlled wear
L. Major*a,
J. M. Lacknerb and
B. Majora
aInstitute of Metallurgy and Materials Science, Polish Academy of Sciences, 30-059 Cracow, Reymonta St.25, Cracow, Poland. E-mail: l.major@imim.pl; Fax: +48-12-2952804; Tel: +48-12-2952800
bJOANNEUM RESEARCH-Materials-Institute for Surface Technologies and Photonics, Leobner Strasse 94, 8712 Niklasdorf, Austria
First published on 26th March 2014
Development of a new generation of multilayer coatings as well as a microstructure understanding of the mechanisms operating at the smallest length scale (nano- and atomic-scale) during wear, opens an avenue for the fabrication of future high-tech functional surfaces. Coatings for the presented work were fabricated by a pulsed laser deposition supported by magnetron sputtering. Microstructure characterization has been performed on as-deposited coatings as well as on coatings after mechanical wear test. Thin foils for detailed TEM microstructure observation were cut directly from the mechanically deformed area, using the FIB technique. Wear mechanisms operating at the small length scale of TiN/Ti/a-C
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H multilayer coatings subjected to mechanical wear was studied by means of transmission electron microscopy (TEM). Cracking of the multilayer systems propagated layer by layer. The highest stress concentration during mechanical uploading was moved through the multilayer coating by breaking only one layer at the time.
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H coatings subjected to mechanical testing, where very thin titanium layers (∼7 nm) were deposited at each TiN/a-C
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H interface.
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H) and titanium nitride (TiN). Pure Ti layers were deposited in an argon (non-reactive) atmosphere, while for the TiN deposition the atmosphere was gradually switched to nitrogen. Additionally, to increase the quality of the coating adhesion and to reduce the residual stress concentration, the thin metallic titanium (Ti) layers were deposited at each interface. Details of the deposition process have been described elsewhere.11 The set of multilayer coatings with a different number of layers and phase ratios at constant coating thicknesses (1.5 μm) were produced. Additionally a-C
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H and TiN single layer coatings were deposited as references. The list of coatings is presented below:
- a-C
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H single layer
- TiN single layer
- 2 × TiN/a-C
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H (4 layers with TiN and a-C
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H with phase ratio 1
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1)
- 8 × TiN/a-C
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H (16 layers with phase ratio 1
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1)
- 32 × TiN/a-C
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H (64 layers with phase ratio 1
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1)
- 8 × TiN/a-C
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H (16 layers with phase ratio 1
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2)
- 8 × TiN/a-C
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H (16 layers with phase ratio 1
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4)
- 8 × TiN/a-C
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H (16 layers with phase ratio 4
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1)
Bio-medical tests were done using smooth muscle cells.12,13 Smooth muscle cells (SMCs) were purchased from Lonza. Each vial had a concentration of 500
000 cells per mL. The cells were stored in liquid nitrogen until use. Before adding cells, the medium was warmed at 37 °C in a water bath. Cells were taken from the liquid nitrogen container and placed for 2–3 min in a 37 °C water bath. SMCs were deposited directly on the surfaces of the coatings. After three days the cells were fixed in 4% paraformaldehyde. Then the cells were permeabilised in a Triton X-100 0.2% detergent for 4 min. The actin cytoskeleton was marked with AlexaFluor Phalloidin, the nucleus with DAPI. Fluorescent dyes were excited with the appropriate laser wavelength, 488 nm for actin cytoskeleton visualization, 405 nm to visualize nucleus of the cell. The cell adhesion to the coating surfaces were observed by confocal microscopy (Carl Zeiss Exciter 5).
The mechanical properties of the coatings were investigated by means of a ball-on-disc (Al2O3 ball with 6 mm radius) mechanical test. Details of the test are given in the table (Table 1).
| Type of the test | Load (N) | Number of cycles | Friction radius (mm) | Line speed (m s−1) |
|---|---|---|---|---|
| Low stress condition (ball-on-disc) | 1 | 20 000 |
5 | 0.06 |
| High stress condition | 5 | 5000 | 4 | 0.05 |
Residual stress distribution was modelled by the finite elements technique. The microstructure of the as-deposited coatings and after the mechanical tests, was studied using scanning (SEM) and transmission (TEM) (TECNAI G2 F20 FEG (200 kV)) electron microscopes, which allows the microstructure observation at the smallest scale, especially in the high resolution mode (high resolution transmission electron microscopy-HRTEM).22 In HRTEM columns of atoms are observed. The chemical composition was characterized by the energy dispersive spectroscopy technique (EDS). Thin foils for TEM analysis were prepared using the focused ion beam technique (FIB-gallium ions) (QUANTA 200 3D Dual Beam), together with the OmniProbe in-situ lift out system. It allowed us to prepare foils directly from places of interest (from mechanically deformed areas-wear tracks).
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H coatings and to describe the microstructure changes and wear mechanisms operating at the small length scale of the described multilayer coatings after mechanical uploading.
The microstructure characterization has been performed on as-deposited coatings, as well as on those after mechanical wear test to observe changes in the microstructure caused by mechanical uploading. The potential application of the presented coatings are cardio-surgical tools.
To improve the adhesion of the coating to the substrate, a titanium (Ti) metallic buffer layer was deposited as a first one. Subsequently an appropriate multilayer structure was produced, where carbon layers were placed sequentially with titanium nitride layers.
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H coating (Fig. 1).
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H single layer coating (Fig. 2a). In the high stress condition the role of the multilayer structure started to be visible. Wear indexes for multilayer coatings were on the same level or even lower than index for the a-C
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H single layer coating (Fig. 2b).
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| Fig. 2 Wear (ball-on-disc) test results: (a) low stress condition (1 N), (b) high stress condition (5 N). | ||
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H interface, which is easily visible at the higher magnification bright field image (Fig. 4). The small amount of the Ti phase between the TiN and a-C
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H layers improves the adhesion of TiN to a-C
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H, which otherwise would be very weak due to a high residual stress. The thickness of the individual titanium layers was approximately 7 nm. The presence of the metallic titanium phase was confirmed by the EDS qualitative chemical analysis and the HRTEM technique in the atomic scale (Fig. 5). The above observations correspond to the deposition process. The pure titanium layers were deposited in an argon atmosphere. As a result, a very thin titanium phase was formed at each TiN/a-C
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H interface. The atmosphere was subsequently switched to a mixture of argon and nitrogen. The nitrogen flow was gradually opened while the argon flow was closed. After reaching the half thickness of the TiN layer, the nitrogen flow was gradually closed, and the argon flow was opened. Similar to before, deposition from the Ti target was finished in an argon atmosphere, allowing the formation of a small amount of Ti phase on the next TiN/a-C
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H interface. Concerning only the TiN phase in the layer, the Ti to N ratio was changed with the distance from the interface. It happened because the gases flow changed with the distance from the interface. The flow was gradually changed.
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Fig. 3 TEM bright field image of an as-deposited 8 × TiN/Ti/a-C : H multilayer coating, together with selected area electron diffraction patterns from selected parts of the coating. | ||
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Fig. 4 TEM bright field image of an as-deposited 8 × TiN/Ti/a-C : H multilayer coating (higher magnification than Fig. 3, revealing thin Ti layers presented at each interface). | ||
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H multilayer coatings after the mechanical wear test. The topography of the coating after the test is presented by the SEM technique (Fig. 6). The place from which the thin foil was prepared is marked on the image. A detailed analysis of the wear mechanisms have been done by the TEM method. One of the main advantages of the described coatings was that cracking has not been performed suddenly. It occurred layer by layer (Fig. 7). The highest, localized stress concentration was moved during the coating deformation from the bottom to the top part of the coating, which was confirmed by numerical modelling (Fig. 8). The layers reunion after movement of individual layers to the closest layer of the same phase was possible by the presence of metallic thin layers at each interface. Another example shows layers motion towards the closed neighbouring layer, however reunion was performed again by thin Ti layers (Fig. 9). Therefore, layer motions were obtained towards the closed neighbour of the same phase, as well as towards the closest neighbouring layer.
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Fig. 6 SEM image of the topography of multilayer an 8 × TiN/Ti/a-C : H coating after the mechanical wear test. | ||
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| Fig. 9 TEM image presenting another example of layers motion and reunions mostly because of the presence of the thin Ti metallic layers. | ||
In the described experiment, to reduce the high residual stress, a metallic buffer layer of 7 nm was deposited at each TiN/a-C
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H interface. Such a composition caused the unusual behavior of the multilayer coating during the mechanical wear, in particular the cracking process. The cracking line, in the described case, because of the presence of very thin Ti layers at each interface, could move through the multilayer coating in the direction of the applied stress by breaking only one layer at a time. Individual layers broke, moved and formed new connection with its neighbour. The mechanism has never been described before in the literature. The layers reunion probably was carried out by moving one broken layer relative to the other along a common interface (in this case-cracking line), while applying a compressive force. The friction heating generated at the interface softens both components, particularly plastically deformed thin Ti layers presented at each interface. The relative motion was then stopped. The connections were formed in the solid state. Anyway, the ‘layers motion’ phenomenon is similar to the edge dislocation motion (Fig. 10).22,23
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| Fig. 10 Attempt to compare the ‘layers-motion mechanism’ to the edge dislocation motion: (a) movement of edge dislocation through the crystal lattice,23 (b) TEM bright field image of the layers motion mechanism. | ||
- Multilayer structure and metallic interlayers in the TiN/Ti/a-C
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H coatings play major roles in controlling the deformation process.
- Propagation of the deformation was realised layer by layer.
- The cracking line, due to the presence of very thin Ti layers at each interface, could move through the multilayer coating in the direction of the applied stress by breaking only one layer at a time.
| This journal is © The Royal Society of Chemistry 2014 |