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Superhard Materials |
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Hard materials can be divided into three
groups (Holeck, 1986)
depending on chemical bonding character: (a) metallic hard materials (borides, carbides, and nitrides of the transition metals, such as TiN, TiC,
TiB2, etc); (b) covalent hard materials (borides, carbides, and nitrides of Al, Si, and B, as well as diamond), and (c) ionic (ceramic)
hard materials (oxides of Al, Zr, Ti, and Be). |
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High Hardness and Elasticity of Nanomaterials |
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Elastic properties of the new superhard materials are fundamental properties of the new phase and must be measured directly (contrary to hardness, which depends on many parameters, including measurement conditions). As a rule covalent hard materials can be obtained under high pressure and high temperature and therefore only in a small amount, usually a few millimeters in size; thus traditional methods for measuring elastic moduli are not applicable. Brillouin scattering has proven to be a unique technique for measuring elastic properties of such small specimens. In our laboratory we ahve been conducting synthesis of new superhard materials for more that ten years. We used Brillouin light scattering (BLS) to measure the elastic properties of superhard phases and nanomaterials and to understand the nature of their anomalous hardness (Zinin, Manghnani. "Elasticity Characterization of Covalent (B-C-N) Hard Materials and Films by Brillouin Scattering" in G. Amarendra and M. H. Manghnani eds. "Recent Advances in Materials Characterization". CRC Press, London, 184-211, 2006). We demonstrated that superhard nanomaterials deviate significantly from this linear trend and exhibit anomalously high Ho values (see Fig. below). This can be attributed to the nanostructure of nanomaterials. For metals, the hardness increases with decreasing grain size (a) as (Hall-Petch effect). Simple extension of the Hall-Petch effect in the nanoscale range gives extremely high hardness and appears not to be valid for nanostructured materials. |
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Vickers
hardness vs. shear modulus for various hard and superhard materials. Data
for BC2N were taken from Refs. (Tkachev, Solozhenko,
Zinin et al., Phys. Rev. B, 68, 052104,
2003) for nc-TiN/-a Si3N4 from Refs. (Manghnani, Tkachev,
Zinin, et al. J. Appl. Phys. 97,
2005), and the rest from Ref. (Teter.
Mater. Res.. Soc. Bull. 23, 22-27,
1998).
The experimental data in the review paper (Teter, 1998) can be best-fitted by a linear trend: Ho = 0.1769G - 2.899 where Ho is the hardness of the crystalline material. Based on the measured shear G moduli of the c-BC2N (238 GPa) the hardness Ho from equation should be 39.2 GPa in contrast to the Ho value of 76 GPa reported by Solozhenko. Thus the SBS measurements demonstrate that superhard nanomaterials deviate sufficiently from the linear trend (see Fig.). We attribute the higher hardness values of the nanocomposite films to the nanostructure.
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Characterization of Hard and Superhard Films by Surface Acoustic Waves |
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The use of hard and superhard coatings is nowadays widely spread in surface
engineering. The system keeps its bulk properties while the film ensures
protection against the environment and achieves properties unattainable
in the substrate alone. Among these layers, one finds hard coatings,
which represent a major improvement in the resistance to wear or abrasion
of numerous industrial components. Their range of applications is large,
extending from intermittent lubricants to more demanding systems such
as coatings on cutting, drilling tools and parts of engine.
The refractory nature of some of these films is used for high temperature
applications, on engine blades for example. |
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Although the use of surface waves is well established for measuring the properties of thin layers, they have rarely been used to investigate hard films. To fill the gap in the theory together with my colleagues Dr. Odile Lefevre (O. Lefeuvre. Ph. D. Thesis. 1998. University of Oxford, Prof. Arthur Every, Prof. Andrew Briggs we have developed a theoretical framework for treating surface wave propagation on such films and demonstrated its application to the characterization of thin hard films (Lefeuvre, Zinin, Briggs, Every. Appl. Phys. Lett. 1998. 72. 856). We are able to distinguish several types of dispersion behaviour, depending on the relative properties of the layer and substrate. When the elastic properties of the layer and the substrate are not very different, the velocity of the pseudo surface wave beyond cut-off increases up to the Rayleigh wave velocity of the layer. When the elastic properties of the two materials are quite dissimilar, the pseudosurface wave tends towards an attenuated interfacial mode. In addition, another mode appears evolving into the Rayleigh wave of the layer material. We show that with this new understanding of surface wave propagation, the characterisation of thin hard films by surface waves is indeed possible.
Left: Two dimensional grey image of the calculated Brillouin spectra of TiN/steel at free TiN surface. |
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This approach has been experimentally applied to hard films belonging to the various dispersion types, including a very fast layer on slow substrate: Si3N4 on GaAs; cBN on Si, films with similar properties to those of the substrate porous oxide layer on aluminium and intermediate systems (barrier films on aluminium (see review M. G. Beghi, A. G. Every, and P. V. Zinin. "Brillouin Scattering Measurement of SAW Velocities for Determining Near-Surface Elastic Properties", in T. Kundu ed., Ultrasonic Nondestructive Evaluation: Engineering and Biological Material Characterizationn, CRC Press, Boca Raton, chapter 10, 581-651, 2003). |
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Diamonds from C60 We used Surface Brillouin Scattering (SBS) technique to study the elastic properties of superhard amorphous carbon, synthesized from C60 under high pressure (13 - 13.5 GPa) and temperature (900+100). This is the first reliable determination of bulk and shear elastic moduli for this type of amorphous carbon material. The measured moduli are found to be close to those of diamond in agreement with the general trend for elasticity, hardness, and density among the carbon phases, demonstrating as well the efficiency of high-pressure fullerene technique for synthesis of sp3-based amorphous carbon materials. Brillouin spectrum of the uperhard amorphous carbon, synthesized from C60 (from Manghnani, Tkachev, Zinin et al. Phys. Rev. B. 64, 121403, 2001).
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