Atomic structure, comparative stability and electronic properties of hydroxylated Ti2C and Ti3C2 nanotubes
Graphical abstract
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Highlights
► Layers of Titanium hydroxicarbides TinCn−1(OH)2 as parent phases for nanotubes. ► Models of TinCn−1(OH)2 nanotubes are designed and studied by DFT-TB method. ► Stability of all TinCn−1(OH)2 nanostructures depends on the type of OH distribution. ► Type of OH ordering determines electronic properties of TinCn−1(OH)2 layers.
Introduction
Titanium carbide (TiC) exhibits an unique combination of excellent physical and chemical properties, such as high melting point, high strength, low electrical resistivity, good anticorrosion and antiwear properties, which make this material highly suitable for various technological applications: as coating, in cutting tools, as reinforcing component in oxide or non-oxide ceramics, in hard alloys, etc. [1], [2], [3], [4]. In turn, nanosized forms of TiC with specific morphologies may provide a wider and diverse ability for further tuning of physical properties and the fabrication of new materials with promising applications and unexpected technological prospects.
Nowadays, a rich set of various physical and chemical pathways for the synthesis of nanostructured TiC has been developed, see for example [5], [6], [7], [8], [9], [10], [11], [12], [13], [14]. Along with quite conventional approaches, such as carbothermal reduction, chemical vapor deposition, sol–gel method, arc discharge technology, etc., also some rather exotic routes are proposed like biotemplate methods which use natural nanoporous bamboo [15] or cotton fibers [16] as both the renewable carbon source and the template in the synthesis of TiC nanowires. As result, a large set of monolithic TiC nanostructures – such as nanoparticles, nanocrystallites, nanowires (nanorods) with different morphology has been synthesized [5], [6], [7], [8], [9], [10], [11], [12], [13], [14], [15], [16].
One of the major challenges in the fabrication of nanostructured TiC materials (as well as of carbides and nitrides of others d metals) is the synthesis of hollow quasi-one-dimensional (tube-like) forms of titanium carbide. The reason is quite obvious: a formation of tube-like nanoforms of isotropic 3D-like crystals with isotropic system of interatomic bonds is much more problematic, than that for the nanotubes of layered compounds (such as graphite, BN, MoS2, etc.) which possess sharply anisotropic systems of interatomic bonding including strong bonds within the layers versus very weak van der Waals-type bonding between the adjacent layers. Indeed, despite a set of theoretical models for monocrystalline TiC nanotubes was proposed [11], [17], [18], [19], any convenient attempt to fabricate such tubular material was absent.
Very recently, a promising possibility to obtain the TiCx nanotubes was demonstrated after the experiments [20], where the graphene-like titanium nanocarbides have been successfully synthesized from so-called MAX phases. These ternary phases (see reviews [21], [22], [23], [24], [25], [26]) with the general formula Mn+1AXn (n = 1, 2, or 3) can be described as intergrowth structures consisting of hexagonal 2D-like blocks [Mn+1Xn] (where M = d metals; X = C or N) alternating with planar atomic sheets A (where A are sp elements such as Al, Ga, Si, Ge, S, etc.) The system of inter-atomic interactions in MAX phases is quite anisotropic with strong directional M–X bonds inside blocks [Mn+1Xn], whereas the bonds between elemental monoatomic sheets A and blocks [Mn+1Xn] are weaker [21], [22], [23], [24], [25], [26]. From these reasons, taking Ti3AlC2 as example, the experiments for the extraction of the most weakly bonded Al from this MAX phase were undertaken. New 2D graphene-like material with nominal composition Ti3C2 was successfully prepared by treatment of Ti3AlC2 powders in HF (Ti3AlC2 + 3HF = AlF3 + 3/2H2 + Ti3C2) and further sonication of the reaction product for exfoliation of nanoblocks Ti3C2 [20]. Moreover, a preliminary evidence for the formation of scrolls from graphene-like Ti3C2 was shown [20].
One may assume that the graphene-like titanium nano-carbides can become successful precursors for the TiCx nanotubes (NTs). The results [20] open also other interesting prospects. A further possibility to update the properties of the proposed TiCx nanotubes arises from their decoration by various atoms or functional groups – e.g., like in experiments [20], where the exfoliated species Ti3C2 were terminated by OH groups and/or by fluorine ions from aqueous environment. Moreover, since about ∼70 synthesized MAX phases are known [21], [22], [23], [24], [25], [26], the preparation of other graphene-like carbides and nitrides of Sc, Ti, V, Cr, Zr, Nb, Mo, Hf and Ta may be proposed, and, in turn, these species may be considered as precursors for rolled up nano-forms of these carbides or nitrides – such as nanoscrolls or nanotubes.
Following these circumstances, in this work we present the atomistic models and report the results of DFTB simulations of stability and electronic properties for TiCx nanotubes, constructed from graphene-like sheets Ti2C and Ti3C2 – as building blocks of Ti2AlC and Ti3AlC2 MAX phases. Besides, the models of hydroxylated Ti2C, and Ti3C2 nanotubes (Ti2C(OH)2, and Ti3C2(OH)2 NTs) are examined, taking into account that the experimentally exfoliated species Ti3C2 were terminated by OH groups. This choice allows to examine the properties of proposed TiCx NTs as a function of their composition (Ti2C versus Ti3C2) and to consider the influence of OH termination on electronic properties and comparative stability of these novel tubular structures.
Section snippets
Models and computational aspects
At first step of our simulations, the free-standing Ti2C, and Ti3C2 layers with the atomic structures of corresponding hexagonal building blocks of Ti2AlC and Ti3AlC2 MAX phases are considered. Afterwards, the atomic models of their hydroxylated forms – hydroxicarbides Ti2C(OH)2, and Ti3C2(OH)2, are constructed. Three main configurations of OH termination of each Ti2C, and Ti3C2 layers are analyzed, when (i) all OH groups are placed at the hollow site (A, Fig. 1) between three neighboring
Ti2C, Ti3C2, Ti2C(OH)2, and Ti3C2(OH)2 planar layers
The relaxed structures of all free-standing Ti2C, Ti3C2, Ti2C(OH)2, and Ti3C2(OH)2 planar layers were found to preserve their integrity after the optimization of their unit cells (Fig. 1). OH termination of Ti2C, Ti3C2 layers (in position A) leads to slight increase of the parameter a for Ti2C(OH)2 and Ti3C2(OH)2 – in agreement with earlier DFT estimations [20] – and the expansion of near-surface C–Ti interplanar distances on about 0.05–0.1 Å comparing to their non-hydroxylated parent phases
Conclusions
The main goal of this work is to evaluate the atomic models and to predict the electronic properties and relative stability for the new family of the quasi-one-dimensional hollow nanostructures of titanium carbides and their hydroxylated forms, whose preparation seems very expectable after the successful synthesis of TiCx graphene-like materials [20].
By means of density-functional tight-binding method, the aforementioned properties for proposed Ti2C, Ti3C2, Ti2C(OH)2, and Ti3C2(OH)2 nanotubes
Acknowledgement
Financial support of the RFBR (Grant 11-03-00156-а) is acknowledged.
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