Abstract

The effects of the vacancy concentration at the cation site of three half-Heuslers, VCoSb, NbCoSb, and TaCoSb, were studied with a combination of two computational methods: density functional theory and Monte Carlo simulations, both linked by a cluster expansion method. Our density functional method allows us to follow a gap opening in the electronic density of states in NbCoSb and TaCoSb as a function of vacancy concentration, starting from a metallic state with the Fermi-level crossing the valence states in the pristine crystal, passing throughout a p-type doped behavior, down to a semiconducting state at 20% of vacancies. In the case of VCoSb, the transition starts from the half-metallic ferromagnetic state, where VCoSb remains half-metallic until it achieves a semiconductor state at V_{0.8}CoSb composition, the transition leading to a magnetic–nonmagnetic crossover. Further increase of vacancies leads to non-polarized in-gap states in V_{0.75}CoSb, and polarized in-gaps in Nb_{0.77}CoSb, while Ta_{0.75}CoSb recovers a metallic behavior but with an n-character. Based on our cluster expansion, we can assert that Ta_{0.8}CoSb is slightly more stable than Nb_{0.8}CoSb, while both are much more stable than V_{0.8}CoSb. Temperature effects were studied through Monte Carlo simulations. The simulations show that, upon cooling, the ground states are hard to recover, and instead metastable states are formed. The vacancy arrangements were scrutinized with the help of suitable order parameters for the lattice vacancy occupation.

Highlights

  • Point defects may appear spontaneously during the manufacturing of a material,[1] and, despite its misleading name, they are sometimes quite desirable in many branches of material science

  • In all three MCoSb systems, the lowest energy atomic configuration corresponds to the same unit cell; among them, the V 0.8CoSb has the highest energy of formation, − 0.48 eV, while Nb0.8CoSb

  • In previous ­CE26 trying to describe the same system, − 0.605 eV of energy was reported in the low-temperature regime, which is higher than the energy we found, indicating that our Monte Carlo (MC) simulation has been able to find a lower energy arrangement of vacancies than the states in Ref. 26

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Summary

Introduction

Point defects may appear spontaneously during the manufacturing of a material,[1] and, despite its misleading name, they are sometimes quite desirable in many branches of material science. When targeting specific physical properties, controlled and selectively induced defects can be used for introducing or tuning desired physical properties.[2]. The presence of vacancy defects can help to tune the power factor or/and the lattice thermal conductivity to deliver a higher figure-of-merit (ZT). One finds reports of vacancies assisting the desired reduction of the lattice thermal conductivity in CuGaTe2,11 while in SnTe-In2Te3,12 Ge9Sb2Te12,13 and -Zn4Sb3,10 the presence of vacancies simultaneously improves the electrical properties and reduces the lattice thermal conductivity. In these improved thermoelectric examples, as in most cases in the field of thermoelectricity, the target was materials with good semiconducting behavior. We present a way to turn a metal (semi-metal) into a semiconductor as well as the possibility of inducing intrinsic n- or p-doping via vacancies

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