First-principles quantum molecular dynamics study of TixZr1−xN(111)/SiNy heterostructures and comparison with experimental results

Abstract The heterostructures of five monolayers B1–TixZr1−xN(111), x = 1.0, 0.6, 0.4 and 0.0 (where B1 is a NaCl-type structure) with one monolayer of a Si3N4-like Si2N3 interfacial layer were investigated by means of first-principles quantum molecular dynamics and a structure optimization procedure using the Quantum ESPRESSO code. Slabs consisting of stoichiometric TiN and ZrN and random, as well as segregated, B1–TixZr1−xN(111) solutions were considered. The calculations of the B1–TixZr1−xN solid solutions, as well as of the heterostructures, showed that the pseudo-binary TiN–ZrN system exhibits a miscibility gap. The segregated heterostructures in which Zr atoms surround the SiyNz interface were found to be the most stable. For the Zr-rich heterostructures, the total energy of the random solid solution was lower compared to that of the segregated one, whereas for the Ti-rich heterostructures the opposite tendency was observed. Hard and super hard Zr–Ti–Si–N coatings with thicknesses from 2.8 to 3.5 μm were obtained using a vacuum arc source with high frequency stimulation. The samples were annealed in a vacuum and in air at 1200 °C. Experimental investigations of Zr–Ti–N, Zr–Ti–Si–N and Ti–Si–N coatings with different Zr, Ti and Si concentrations were carried out for comparison with results obtained from TixZr1−xN(111)/SiNy systems. During annealing, the hardness of the best series samples was increased from (39.6 ± 1.4) to 53.6 GPa, which seemed to indicate that a spinodal segregation along grain interfaces was finished. A maximum hardness of 40.8 GPa before and 55 GPa after annealing in air at 500 °C was observed for coatings with a concentration of elements of Si  (7–8) at.%, Ti  22 at.% and Zr  70 at.%.

[1]  M. Gu,et al.  Study on the superhardness mechanism of Ti–Si–N nanocomposite films: Influence of the thickness of the Si3N4 interfacial phase , 2005 .

[2]  Shang Da-Shang,et al.  Resistance switching in oxides with inhomogeneous conductivity , 2013, 1304.3290.

[3]  D. Vanderbilt,et al.  Soft self-consistent pseudopotentials in a generalized eigenvalue formalism. , 1990, Physical review. B, Condensed matter.

[4]  L. Keer,et al.  Synthesis and structure of smooth, superhard TiN/SiNx multilayer coatings with an equiaxed microstructure , 2001 .

[5]  V. Beresnev,et al.  Effect of the preparation conditions on the phase composition, structure, and mechanical characteristics of vacuum-Arc Zr-Ti-Si-N coatings , 2011 .

[6]  A. Pogrebnjak,et al.  Hard Nanocomposite Coatings, Their Structure and Properties , 2012 .

[7]  F. Lévy,et al.  Structure, morphology and electrical properties of sputtered Zr–Si–N thin films: From solid solution to nanocomposite , 2006 .

[8]  S. Vepřek,et al.  A concept for the design of novel superhard coatings , 1995 .

[9]  P. Zeman,et al.  Hard a-Si3N4/MeNx Nanocomposite Coatings with High Thermal Stability and High Oxidation Resistance , 2007 .

[10]  J. Procházka,et al.  Different approaches to superhard coatings and nanocomposites , 2005 .

[11]  M. V. Kaverin,et al.  Phase Composition, Thermal Stability, Physical and Mechanical Properties of Superhard on Base Zr‐Ti‐Si‐N Nanocomposite Coatings , 2010 .

[12]  V. M. Beresnev,et al.  Nanocoatings Nanosystems Nanotechnologies , 2012 .

[13]  L. Hultman,et al.  Self-organization during Growth of ZrN/SiNx Multilayers by Epitaxial Lateral Overgrowth , 2013 .

[14]  J. Musil Hard and superhard nanocomposite coatings , 2000 .

[15]  R. F. Zhang,et al.  Origin of the hardness enhancement in superhard nc-TiN/a-Si3N4 and ultrahard nc-TiN/a-Si3N4/TiSi2 nanocomposites , 2007 .

[16]  A. D. Pogrebnyak,et al.  REVIEWS OF TOPICAL PROBLEMS: Structures and properties of hard and superhard nanocomposite coatings , 2009 .

[17]  L. Hultman Synthesis, Structure, and Properties of Super-Hard Superlattice Coatings , 2006 .

[18]  Ruifeng Zhang,et al.  Understanding why the thinnest SiN x interface in transition-metal nitrides is stronger than the ideal bulk crystal , 2010 .

[19]  Hans Söderberg,et al.  Nanostructure formation during deposition of TiN SiNx nanomultilayer films by reactive dual magnetron sputtering , 2005 .

[20]  S. Vepřek,et al.  Industrial applications of superhard nanocomposite coatings , 2008 .

[21]  S. H. Sheng,et al.  Superhard nanocomposites: Origin of hardness enhancement, properties and applications , 2010 .

[22]  P. Turchi,et al.  Comparative first-principles study of TiN/SiNx/TiN interfaces , 2012 .

[23]  A. P. Shpak,et al.  Effect of thermal annealing in vacuum and in air on nanograin sizes in hard and superhard coatings Zr-Ti-Si-N. , 2012, Journal of nanoscience and nanotechnology.

[24]  M. V. Kaverin,et al.  Triboengineering properties of nanocomposite coatings Ti-Zr-Si-N deposited by ion plasma method , 2012 .

[25]  M. Ferenets,et al.  Thin Solid Films , 2010 .

[26]  M. Odén,et al.  Thermal stability, microstructure and mechanical properties of Ti1 − xZrxN thin films , 2008 .

[27]  J. Musil,et al.  Hard nanocomposite coatings: Thermal stability, oxidation resistance and toughness , 2012 .

[28]  Lili Wang,et al.  Structures, mechanical properties and thermal stability of TiN/SiNx multilayer coatings deposited by magnetron sputtering , 2009 .

[29]  I. Petrov,et al.  Interface structure in superhard TiN-SiN nanolaminates and nanocomposites : film growth experiments and ab initio calculations , 2007 .

[30]  J. Koehler Attempt to Design a Strong Solid , 1970 .

[31]  Burke,et al.  Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.

[32]  J. Molina-Aldareguia,et al.  Epitaxial stabilization of cubic- SiNx in TiN/SiNx multilayers , 2006 .

[33]  Fadei F. Komarov,et al.  Adhesive strength, superhardness, and the phase and elemental compositions of nanostructured coatings based on Ti-Hf-Si-N , 2012 .

[34]  Siegfried Schmauder,et al.  Comput. Mater. Sci. , 1998 .

[35]  R. F. Zhang,et al.  Friedel oscillations are limiting the strength of superhard nanocomposites and heterostructures. , 2009, Physical review letters.

[36]  A. Curioni,et al.  Efficient linear scaling geometry optimization and transition-state search for direct wavefunction optimization schemes in density functional theory using a plane-wave basis , 2003 .

[37]  M. M. Chaudhri,et al.  Nanohardness of high purity Cu (111) single crystals: The effect of indenter load and prior plastic sample strain , 2010 .

[38]  M. Odén,et al.  Growth and characterization of TiN/SiN(001) superlattice films , 2007 .

[39]  H. Monkhorst,et al.  SPECIAL POINTS FOR BRILLOUIN-ZONE INTEGRATIONS , 1976 .

[40]  P. Zeman,et al.  Hard amorphous nanocomposite coatings with oxidation resistance above 1000°C , 2008 .