Elsevier

Acta Materialia

Volume 187, 1 April 2020, Pages 84-90
Acta Materialia

Full length article
Structural failure of layered thermoelectric In4Se3-δ semiconductors is dominated by shear slippage

https://doi.org/10.1016/j.actamat.2020.01.045Get rights and content

Abstract

In4Se3-δ semiconductors exhibit high zT as an n-type TE material, making them promising materials for thermoelectric (TE) applications. However, their commercial applications have been limited by the degradation of their mechanical properties upon cyclic thermal loading, making it important to understand their stress response under external loadings. Thus we applied molecular dynamics (MD) simulations using a density functional theory (DFT) derived force field to investigate the stress response and failure mechanism of In4Se3-δ under shear loading as a function of strain rates and temperatures. We considered the most plausible slip system (001)/<100> based on the calculations. We find that shear slippage among In/Se layered structures dominates the shear failure of In4Se3-δ. Particularly, Se vacancies promote disorder of the In atoms in the shear band, which accelerates the shear failure. With increasing temperature, the critical failure strength of In4Se3 and the fracture strain of In4Se3 decrease gradually. In contrast, the fracture strain of In4Se2.75 is improved although the ultimate strength decreases as temperature increases, suggesting that the Se vacancies enhance the ductility at high temperature. In addition, the ultimate strength and the fracture strain for In4Se2.75 increase slightly with the strain rate. This strain rate effect is more significant at low temperature for In4Se2.75 because of the Se vacancies. These findings provide new perspectives of intrinsic failure of In4Se3-δ and theory basis for developing robust In4Se3-δ TE devices.

Introduction

Thermoelectric (TE) devices can directly convert the heat from automotive exhausts into electricity, which is of great significance for energy sustainability [1,2]. Many efforts have been made to improve the low efficiency of TE energy conversion, which is characterized by the figure of merit, zT=S2σT/κ, where S is the Seebeck coefficient, σ is the electrical conductivity, T is the absolute temperature, and κ is the thermal conductivity [2]. The zT could be improved by optimizing the power factor (PF=S2σ) and reducing the thermal conductivity (κ) through introducing point and planar defects (vacancies, doping, elemental substitutions and nano-engineering) in various high-performance TE materials such as Mg2(Si, Ge, Sn) [3], [4], [5], [6], CoSb3 [7], [8], [9], Bi2Te3 [10], [11], [12], PbTe [13], [14], [15], SnSe [16], [17], [18], Zintl phases [19,20], and Half-Heusler alloys [21], [22], [23]. The engineering application of TE materials requires mechanical robustness that can undergo cycling thermal stress in a temperature gradient and can resist crack opening or failure of devices from vibrations. Unfortunately, thermo-mechanical loadings can cause the degeneration of the mechanical properties, leading to the failure of TE devices [24], [25], [26], [27]. Thus, it is essential to obtain an in-depth understanding of how mechanical properties of these TE materials behave in engineering applications.

A TE device requires one p-type and one n-type leg which are equally important for engineering applications. The n-type TE material In4Se3-δ (self-doping by Se deficiency) was reported as a promising candidate for applications in the mid-temperature range (500 to 900 K) with a zT value of 1.48 at 705 K. This high zT value is attributed to its highly anisotropic crystal structure arising from a disordered two-dimensional crystalline sheets coupled with a charge density wave (CDW) instability arising from its distinctive electronic structure [28], [29], [30]. Many efforts have been made to improve the thermoelectric and mechanical properties of In4Se3-δ. Zhu et al. [31] reported that the electrical conductivity and thermal conductivity of polycrystalline In4Se3-δ compounds can be controlled by adjusting Se vacancies, with the zT value reaching ~1.0 for δ = 0.65 and 0.8. Li et al. successfully strengthened the flexural strength of In4Se2.65 TE material by 40% through introducing the uniformly distributed TiC nanoparticles into In4Se2.65 composites [32]. In addition, many theoretical predictions have been made on the electronic and thermal transport properties of In4Se3-δ. Thus, Luo et al. [33] used first-principles simulations to show that the site and concentration of Se vacancies strongly effects the thermoelectric performance of In4Se3. Ji et al. [28] used molecular dynamics (MD) simulations to find that phonon propagation is strongly dependent on the Se deficiency along the In/Se chain direction, which is pivotal in optimizing TE performance.

We have applied density functional theory to determine that the (001)/<100> is the easiest slip system of In4Se3 under shear stress among these slip systems ((001)/<100>, (100)/<010>, (010)/<001>, (110)/<100> and (−110)/<110>) [34]. Nevertheless, such DFT studies are limited to hundreds of atoms and zero temperature so that the intrinsic failure mechanism of In4Se3 at higher temperatures as a function of Se deficiency and strain rate remains unknown.

This work determines the deformation mechanism of the In4Se3-δ TE materials under shear loading along (001)/<100> slip system, including the effects of temperature and strain rate. Applying large-scale MD simulations to finite shear deformation on single crystal In4Se3-δ along the (001)/<100> slip system, we find shear slippage in In/Se layered structures dominates the shear fracture of In4Se3-δ and that Se vacancies accelerate this failure process. Increasing temperatures have a dramatic influence on the ultimate strength and the fracture strain. The strain rate has a slight effect on the mechanical properties but it is more significant at low temperature for In4Se2.75 because of the presence of Se vacancies.

Section snippets

Methodology

All MD simulations were conducted using the large-scale atomic/molecular massive parallel simulator (LAMMPS) open-source software [35,36]. The atomic interaction in In4Se3 were described using the force field developed previously. A Morse bond term was used to describe the valence pair interactions and the cosine-squared angle term was applied to describe the three-body interactions. The elastic properties and thermal conductivity of In4Se3 are predicted accurately using this force field [28].

Atomic structure of In4Se3-δ

The In4Se3 binary compound crystallizes in the Pnnm orthorhombic space group (No. 58) with 28 atoms per cell (see Fig. 1a). It has lattice parameters of a = 15.297 Å, b = 12.308 Å, and c = 4.081 Å [40,41]. The In1, In2 and In3 atoms as In1.667+ form In-In metallic bonds (2.77 Å average) which connect to Se atoms by In-Se covalent bonds (2.62 to 2.80 Å). This forms the In/Se layered structures stacked along the 〈100〉 direction by van der Waals forces. Specifically, the structure is composed of

Conclusion

In summary, we employed MD simulations to investigate the fracture mechanism of layered thermoelectric In4Se3-δ under shear loading along the most plausible (001)/<100> slip system. We found that the shear slippage among In/Se layered structures dominates the structural destruction in In4Se3-δ systems, while the In/Se sub-structures (the In/Se chains, the In/Se pentagon frameworks and the In1-In2-In3 trios) remain intact. The Se vacancies soften the structure and weaken the mechanical

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

This work was supported by the National Natural Science Foundation of China (No. 51972253, 51772231); the Hubei Provincial Natural Science Foundation of China (2018CFB646); and the Fundamental Research Funds for the Central Universities (No. WUT 2019IVA055, 2019IB006). We acknowledge Sandia National Laboratories for distributing the open-source MD software LAMMPS. Wag was supported by the US NSF (CBET-1805022).

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