Electro-structural correlations, elastic and optical properties among the nanolaminated ternary carbides Zr2AC

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Abstract

We have performed ab initio calculations for the nanolaminates Zr2AC (A = Ti, In, Tl, Si, Ge, Sn, Pb, P, As, S) ceramics to study their electronic structure, elastic and optical properties. In this work, we used the accurate augmented plane wave plus local orbital method with density functional theory to find the equilibrium structural parameters, dielectric functions and to compute the full elastic tensors. The obtained elastic constants were used to quantify the stiffness of the Zr2AC phases and to appraise their mechanical stability. The relationship between elastic, electronic and valence electron concentration is discussed. Our results show that the bulk modulus and shear modulus increase across the periodic table for Zr2AC. Furthermore, trends in elastic stiffness are well explained in terms of electronic structure analysis, as occupation of valence electrons in states near the Fermi level of Zr2AC. We show that increments of bulk moduli originate from additional valence electrons filling states involving Zr d–A p. We show also that Zr d–A p hybridizations are located just below the Fermi level and are weaker bonds than the Zr d–C p hybridizations, which are deeper in energy. As a function of the p-state filling of the A element the Zr d–A p bands are driven to deeper energy. The optical spectra were analyzed by means of the electronic structure, which provides theoretical understanding of the conduction mechanism of these ceramics.

Introduction

The Mn+1AXn (MAX) phases (n = 1–3) are layered hexagonal compounds, in which near close-packed layers of M (early transition metals) are interleaved with layers of group A element (mostly IIIA and IVA), with the X-atoms (C and/or N) filling the octahedral sites between the M layers. The MAX phases represent a class of technologically important solids exhibiting unusual properties associated with both metals and ceramics [1]. Generally, the Mn+1AXn phases are machinable, [2] exhibit good damage tolerance, [3] have excellent thermal shock resistance, [4] good corrosion resistance, [5] and they are good thermal and electrical conductors [6], [7]. These materials gained renewed interest since Barsoum and co-workers [8] succeed to synthesize single phase, bulk dense samples of Ti3SiC2. Afterwards, many of the roughly 60 Mn+1AXn phases known to date have been studied both experimentally and theoretically [9], [10], [11]. However, individual properties vary from phase to phase. Only limited data are available describing the systematic dependence of the properties on the electronic structure. It has been suggested from ab initio calculations [12] that M2AC (M = Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W and A = Al, Ga, Ge and Sn) can be classified into two groups: one where the bulk modulus of the binary MC is conserved and the other for which the bulk modulus is decreased. However, the same authors [13] have questioned their own results, the description of the binary carbides MC being very sensitive to the choice of the projector augmented wave (PAW) potentials they used. In the same way, Schneider et al. reported that the bulk modulus increases with p electron concentration at the M site for Ta2AC [14]. Recently, Hug [15] has studied the electronic properties among ternary carbides Ti-based compounds. All these phases are shown, except for A = Si, P and As, to be stable, a behavior originating from the particularities of the hybridization scheme in these compounds (Ti d–A p and Ti d–C p hybrids). More recently, we have suggested that the 211 M2SnC (M = Ti, Zr, Hf and Nb) MAX phases hold back about 69% of the bulk modulus of the corresponding binary carbides, a value close to 2/3. Knowing that the bulk moduli of M3SiC2 are 3/4 of the corresponding MC, it is curious to remark that the bulk moduli of Mn+1ACn are pretty close to n+1/n+2 of the corresponding binary carbides for n = 1 and 2. Such a phenomenological relation will give 4/5 for the bulk moduli of M4AC3 compared to the related MC ones [16].

Thus, in the present paper, we focus our intention on the physical properties of nanolaminate Zr2AC with A = Ti, In, Tl, Si, Ge, Sn, Pb, P, As, and S by mean of full-potential first principles calculations. Specifically, we address the crystal parameters, electronic structure, mechanical behavior and optical properties of these compounds. It is our ambition to contribute towards understanding the relationship between the elastic properties and electronic structure as a function of valence electron population of A element. The elastic properties are of particular interest as they determine the mechanical stability of the material and important macroscopic properties such as hardness, lubrification, friction, and machinability. The electronic structure and chemical bonding investigation will then provide an overall view of electro-structural information that is needed for tailoring and improving the electronic features of these materials. We have to point out that many theoretical calculations have been carried out on the electronic structures of MAX phases, but the optical properties of the MAX phases have not received adequate attention from neither experimentalists nor theorists.

Section snippets

Theoretical method and crystal structure

The present calculations were performed using an all-electron full-potential (linearized) augmented plane waves plus local orbitals (FP-L/APW + lo) method [17], based on the density functional theory (DFT) [18]. The exchange correlation potential was computed with the Wu and Cohen generalized gradient approximation (GGA-WC) [19]. The maximum value lmax for the wave functions expansion inside the atomic spheres is limited to 10. To achieve the energy eigenvalues convergence, the wave functions

Structural properties

To investigate the ground-state properties, we computed the equilibrium lattice configurations of Zr2AC phases at first optimized lattice parameters for a, c and ZM are summarized in Table 1 as well as the experimental data [22] for comparison. As a general remark, it can be note that all the Zr2AC compounds, are intrinsically stable. The deviations are estimated to be about 0.1% and 0.8% for a and c compared to available experimental work. The formation energies ΔEf of these MAX phases,

Elastic properties

The elastic stiffness determines the response of the crystal to an externally applied strain (or stress) and provides information about the bonding characteristics, mechanical and structural stability. In general, estimating elastic constants from first principles calculation is really tough because it requires accurate methods to evaluate the total energy or stress accompanying strain. Fortunately, state of the art first principles computational modeling permits us to reproduce the elastic

Electronic properties

In order to explain the electronic structure, we have calculated the total density of state (TDOS) using optimized geometry at equilibrium volume. As shown in Fig. 4, the DOS around the Fermi level (EF) generally lies in a dip. This location may split bonding and antibonding states giving rise to stranger cohesion, the structure stability [41] and higher bulk modulus. However, the TDOS of the alloys with s2p3 A atoms presents a sharp peak at EF a configuration which is often associated with

Optical properties

A study of the optical properties of solids has been an interesting research topic, both in basic research as well as for industrial applications. While for the former the origin and nature of different excitation processes are of fundamental interest, the latter can make use of them in many optoelectronic devices. Therefore optical properties bring together experiment and theory. The calculation of ɛ2(ω) requires energy eigenvalues and electron wave functions. These are natural outputs of a

Conclusion

In summary, this work reports on a study of electro-structural correlation, elastic and optical properties of Zr2AC (A = Ti, In, Tl, Si, Ge, Sn, Pb, P, As, S) through first principles all-electron full-potential linearized augmented plane wave calculations. It has been shown that the structural parameters obtained after relaxation are in good agreement with the experimental ones. Our results show that the increase of p electrons from A elements when moving rightwards along the periodic table

Acknowledgments

The calculations using Wien2k code have been performed on the Interuniversity Scientific Computing Facility (ISCF), installed at the FUNDP for which the authors gratefully acknowledge the financial support of the F.R.S.-FRFC and of the “Loterie Nationale” under Contract No. 2.4.617.07.F, and of the FUNDP (Namur, Belgium). M.B.K and S.G.S acknowledge F. Wautelet (ISCF-FUNDP) for permanent computer assistance. Alberto Otero de la Roza from Universidad de Oviedo (spain) is acknowledged for

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