Elsevier

Ceramics International

Volume 40, Issue 9, Part A, November 2014, Pages 14453-14462
Ceramics International

Tensile and fracture process of the TiN/VN interface from first principles

https://doi.org/10.1016/j.ceramint.2014.07.016Get rights and content

Abstract

We have conducted a comprehensive first-principles investigation of tensile and fracture process of the TiN/VN interface by focusing on the strain–stress relationships, the ideal tensile strength and bonding breaking process. The deformation analysis reveals that all bonds are extended at the initial stage until the critical point of fracture is reached. The fracture occurs between the second and third layers on the VN side in both (111) and (001) interfaces and the interaction of potential bonds of facture weakens gradually with the increment of strain during the tensile process. By using several analytical techniques, we identify a charge transfer in both the TiN and VN layers near to interface at the points of fracture during the tensile process, which plays a crucial role in affecting the fracture process. We further demonstrate that the fracture of the TiN/VN interface occurs within the VN and that adhesion energy cannot be simply used to represent tensile strength.

Introduction

Transition–metal–nitride multilayered coatings have received a considerable amount of interest over the past decades, largely because their properties are applicable for various industrial applications [1], [2], including good wear resistance, high thermal and chemical stability. A representative example is that the coatings such as TiN/VN and TixV1−xN can exhibit a high hardness of over 50 GPa and thus hold substantial promise for dry milling, drilling and turning [3], [4], [5]. Moreover, multilayered TiN/VN coatings show significantly enhanced friction and wear performance as compared to their mononitride coatings TiN and VN and the TiAlN/CrN [6], [7], [8]. All the improved properties, including post-processing behavior, rely critically on specific atomic structure, local chemistry, and local bonding at interface [9].

To understand origins behind mechanical properties of multilayered coatings, it is of fundamental significance to investigate tensile behavior because it is strongly connected to the onset of fracture and dislocation nucleation. In particular, multilayered coatings can often downgrade properties of materials during tensile process. However, few works have been conducted on the deformation mechanism of the multilayered coatings. For instance, Rzepiejewska-Malyska et al. [10] found, by the application of in-situ nano-indentation in scanning electron microscopy, a mixture of two modes where TiN deforms through grain boundary sliding and CrN through densification and material flow. Latella et al. [8] used in-situ tensile tests to introduce strains in coatings, and found that the stressed coatings show a mix of cracks perpendicular to tensile axis. Despite the efforts, it remains difficult to extract sufficient information on the process and ultimate geometry particularly at the atomic scale because of complex in directly visualizing variation of interfacial bondings in multilayered coatings.

One way out to complement the experiments so as to develop a general knowledge of the technologically relevant multilayered coatings is through atomistic simulation. To this end, density functional theory (DFT) calculations have often been applied [11]. Liao et al. [12] established a relationship between mechanical property and electronic structure for ternary M2AC (M=Ti, V, Cr, A=Al, Si, P, S) carbides from first principles. Stampfl et al. [13] investigated formation, atomic and electronic structure of metal–nitride interfaces and found that the growth of TiN on VN is energetically favorable. Zhang et al. [14], [15] investigated the tensile and fracture process of the Al/TiN interface, and found that the Al/TiN(001) interface has a smaller work of adhesion and larger tensile strength than the Al/TiN(111) interface. Moreover, Zhang et al. [16] investigated superhard mechanism of AlN/TiN system and attributed the hardness enhancement to formation of semicoherent interface. Considering the relevance of fracture process in affecting mechanical property of nano-multilayers, there have been few investigations of such process particularly at the atomic scale, although mechanical strength of single-phase metals or ceramics has been investigated [17], [18], [19], [20], [21], [22], [23]. Here, we conduct a systematic first-principles investigation of ideal tensile stress and fracture behaviors of the TiN/VN interface. To our knowledge, this is a first systematic report on tensile fracture of the TiN/VN interface. We identify an upper limit to the true yield stress and establish a correlation between the fracture properties of multilayers and their electronic structures.

The rest of this paper is structured as follows. Section 2 describes the computational method and details in this study. The major results of this paper are presented in Section 3, where the results of tensile simulation of TiN/VN interface are provided and the strain–stress relationship is discussed. The TiN/VN interfaces considered are divided into two groups, based on the orientations. The results on (111)-oriented interface are presented in Section 4 and those on (001)-oriented one in Section 5. We provide concluding remarks in Section 6.

Section snippets

Computational details

Calculations were performed using the Cambridge Sequential Total Energy Package (CASTEP) within the framework of DFT [24]. The pseudopotential [25] was employed for describing the electron–ion interaction and the generalized gradient approximation of Perdew and Wang (PW91) [26] was applied to address exchange-correlation functional. Ground-state charge densities were calculated self-consistently using a Pulay-type mixing scheme [27]. Single-particle Kohn–Sham wave functions were expanded using

Atomic models

The TiN/VN interface maintains the stacking sequence as that in constituent bulks, that is, the interfacial atoms of TiN are straight above the third-layer atoms of VN [30]. We first investigate interfaces without stress in the direction perpendicular to interface. Fig. 1 shows the models applied for the tensile simulations, where the (001) and (111) planes of TiN are sketched only for simplicity. Moreover, the structures and properties of TiN(001), TiN(111), VN(001), VN(111), and

Local deformation analysis

To understand mechanism of deformations, each interlayer parallel to interface at an energy strain stage has been systematically analyzed, as shown in Fig. 3. When the stress is imposed, the interlayer distance of TiN and VN layers and Tisingle bondN interfacial bonds are extended. However, difference occurs between the deformation TiN and VN layers: the deformation of VN interlayer at each stage is severer than that of TiN, in line with the fact that elastic constant C11 of VN is smaller than that of

Local deformation analysis

Fig. 7 shows strain as a function of each interlayer for the TiN/VN (001) system. As seen in the (111) system, deformation behavior of the V32 differs from that of other interlayers when the system is extended: the deformation of VN2–VN3 interlayer at each strain stage is remarkably severer than that of rest of interlayers. At the initial stage with a strain of 4%, the interlayer distance for the VN, TiN, and VT interface are all extended. When the strain reaches up to 8%, the V32 suffers the

Conclusions

We have performed a first-principles study of the tensile and fracture process of the TiN/VN interface, aiming at estimating ideal tensile strength and offering atomic details of the bond-breaking process. We find that the TiN/VN (111) system shows a higher Wad and ideal tensile strength than the (001) system, demonstrating that the texture orientation plays an essential role in enhancing mechanical properties. Moreover, the TiN/VN(111) system has a larger Wad (6.57 J/m2) than VN (111) single

Acknowledgments

This study is supported in part by National Science Foundation of China (NSFC) under Grant no. 11302141 and Specialized Research Fund for Doctoral Program of Higher Education (New teachers) under Grant no. 20130181120118. X.P. appreciates the financial supports from NSFC (Grant no. 11332013). D.Y. and Y.Q. acknowledge European Commission for financial funding of research through the EU FP7 M3-2S project and the permission for using the CASTEP code as a registered academic license of CASTEP

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