Abstract:A series of nanoindentation tests has been carried out with TiO2 films produced by physical vapour deposition (PVD) under different conditions. Films with different microstructures and crystallographic structures have been prepared by changing experimental parameters such as the temperature of the substrate, the deposition angle (by the so-called glancing angle physical vapour deposition, GAPVD) or by exposing the growing film to a beam of accelerated ions. The obtained results of hardness and Young's modulus … Show more
“…These data are also presented in Figure 3a and b, in order to better compare the different values of hardness and elastic modulus, respectively. This figure clearly shows that hardness and elastic modulus depend on the deposition angle, a result that agrees with previous results for TiO 2 PV-OAD coatings [19,21]. Common features of PV-OAD thin films, including the TiO 2 -SiO 2 multilayers studied here, are that both the tilting angle of nanocolumns and the void space increase with the deposition angle (c.f., Figure 1) [2,3,6,7].…”
Section: Hardness and Elastic Modulussupporting
confidence: 91%
“…However, mechanical properties such as hardness, elastic modulus or interfacial cohesion of this type of nanostructured multilayer TiO 2 -SiO 2 coatings have not been reported so far. In previous works, the mechanical properties of TiO 2 nanocolumnar coatings made by PV-OAD were investigated as a function of the zenithal angle of deposition [19,21], finding a strong dependence between the mechanical response and the deposition angle. The objective of the present work is to characterize the mechanical response of multilayer coatings formed by a different number layers of TiO 2 and SiO 2 stacked in the form of distinct microarchitectures where the tilted nanocolumns in successive layers present slanted, zigzag or chiral configurations.…”
Abstract. This paper presents a study of the mechanical properties and an evaluation of damage mechanisms of nanocolumnar TiO 2 -SiO 2 multilayer coatings prepared by physical vapour oblique angle deposition at different configurations (slanted, zigzag or chiral) and two zenithal evaporation angles (70º or 85º). The characterization at micro-and nano-metric length scales of the mechanical properties of the multilayers has been carried out by nanoindentation and nanoscratch tests, while the morphological evaluation the surface and sub-surface damages produced with a sharp indenter and the adhesive and/or cohesive failures between coating and substrate have been investigated by field emission scanning electron microscopy and focused ion beam, respectively. The obtained results have shown that the main processing parameters controlling the mechanical response of the different multilayers is the zenithal angle of deposition and the number of layers in the multilayer stack, while the coating architecture had only a minor effect on the mechanical response. This analysis also revealed a higher resistance to scratch testing and a brittle failure behaviour for the low zenithal angle coatings as compared with the high angle ones.
“…These data are also presented in Figure 3a and b, in order to better compare the different values of hardness and elastic modulus, respectively. This figure clearly shows that hardness and elastic modulus depend on the deposition angle, a result that agrees with previous results for TiO 2 PV-OAD coatings [19,21]. Common features of PV-OAD thin films, including the TiO 2 -SiO 2 multilayers studied here, are that both the tilting angle of nanocolumns and the void space increase with the deposition angle (c.f., Figure 1) [2,3,6,7].…”
Section: Hardness and Elastic Modulussupporting
confidence: 91%
“…However, mechanical properties such as hardness, elastic modulus or interfacial cohesion of this type of nanostructured multilayer TiO 2 -SiO 2 coatings have not been reported so far. In previous works, the mechanical properties of TiO 2 nanocolumnar coatings made by PV-OAD were investigated as a function of the zenithal angle of deposition [19,21], finding a strong dependence between the mechanical response and the deposition angle. The objective of the present work is to characterize the mechanical response of multilayer coatings formed by a different number layers of TiO 2 and SiO 2 stacked in the form of distinct microarchitectures where the tilted nanocolumns in successive layers present slanted, zigzag or chiral configurations.…”
Abstract. This paper presents a study of the mechanical properties and an evaluation of damage mechanisms of nanocolumnar TiO 2 -SiO 2 multilayer coatings prepared by physical vapour oblique angle deposition at different configurations (slanted, zigzag or chiral) and two zenithal evaporation angles (70º or 85º). The characterization at micro-and nano-metric length scales of the mechanical properties of the multilayers has been carried out by nanoindentation and nanoscratch tests, while the morphological evaluation the surface and sub-surface damages produced with a sharp indenter and the adhesive and/or cohesive failures between coating and substrate have been investigated by field emission scanning electron microscopy and focused ion beam, respectively. The obtained results have shown that the main processing parameters controlling the mechanical response of the different multilayers is the zenithal angle of deposition and the number of layers in the multilayer stack, while the coating architecture had only a minor effect on the mechanical response. This analysis also revealed a higher resistance to scratch testing and a brittle failure behaviour for the low zenithal angle coatings as compared with the high angle ones.
“…This deposition technique produces anisotropic porous thin films characterized by a tilted columnars microstructure resulting from shadowing effects during the growth process [16][17][18] . The nanocolumns tilting angle and porosity of these films increase gradually with the deposition angle while, simultaneously, the number of nanocolumns per unit area decreases 19,20 . In some materials like SiO2 the tilted nanocolumns tend to aggregate in the form of parallel nanochannels arranged perpendicular to the direction of the incoming flux.…”
mentioning
confidence: 97%
“…Similar experiments carried out with G-TiO2/PDMS foils showed a similar decreasing trend, although in this system no significant differences were found by bending along the x or y axis (see S5). This different behavior can be linked with the low tendency of the TiO2-GLAD films to develop bundles of nanocolumns 19,20 and stresses the importance of the film nanostructure for the control of the micropatterning processes. Another interesting feature of the G-SiO2/PDMS system is that the average crack spacing is independent of the thin film thickness.…”
In general, cracking of thin films is synonym of irreversible damage, delamination and/or device failure. Nevertheless, under certain well controlled conditions, a tensile stress applied to a supported film can induce the development of a regular pattern perpendicular to the resulting strain 11,12 . For example, patterns of cracks produced by uniaxial straining of plasma surface
“…The opposite trend is seen with the 55% titaniadoped samples (black, upward triangles); again, with the exception of the 400°C sample. This is most likely due to the abundance of titania, which is known to have a low crystallization temperature and a high Young's modulus [36,37]. The two titania-doped samples heat-treated at 400°C were produced at the same time; they were most likely heat-treated together and may not have been fully heat-treated.…”
The current generation of advanced gravitational wave detectors utilize titania-doped tantala/silica multilayer stacks for their mirror coatings. The properties of the low-refractive-index silica are well known; however, in the absence of detailed direct measurements, the material parameters of Young's modulus and coefficient of thermal expansion (CTE) of the high refractive index material, titania-doped tantala, have been assumed to be equal to values measured for pure tantala coatings. In order to ascertain the true values necessary for thermal noise calculations, we have undertaken measurements of Young's modulus and CTE through the use of nanoindentation and thermal-bending measurements. The measurements were designed to assess the effects of titania-doping concentration and postdeposition heat-treatment on the measured values in order to evaluate the possibility of optimizing material parameters to further improve thermal noise in the detector. Young's modulus measurements on pure tantala and 25% and 55% titania-doped tantala show a wide range of values, from 132 to 177 GPa, which are dependent on both titania concentration and heat-treatment. Measurements of CTE give values of 3.9 0.1 × 10 −6 K −1 and 4.9 0.3 × 10 −6 K −1 for 25% and 55% titania-doped tantala, respectively, without dependence on post-deposition heat-treatment.
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