Abstract

In this work, we have evaluated how CoNbSn, IrNbSn, and RhNbSn half Heusler alloys respond to temperature change and the accompanying lattice vibrations as a cubic crystal. There are reports in the literature for CoNbSn with which we compared our result; there are, however, no reports for the other two alloys except for their Debye temperature obtained via machine learning, and our results compare well. Considering that results in the literature for IrNbSn and RhNbSn are scanty, we first computed the alloys' structural and electronic properties to establish their structural stability using the density functional theory and generalised gradient approximation as implemented in the quantum espresso computational suite. We confirmed the equilibrium lattice structure by exploring the three possibilities for a half Heusler alloy and fitting the results to the state's Murnaghan equation. The negative formation energies obtained supports experimental simulation of the alloys. Results from the lattice dynamics and thermodynamic evaluation show that the alloys favour ionic bonding and are ductile. The Debye temperature positions IrNbSn to be the most promising material for thermoelectric application because it has the least Debye temperature; hence it is supposed to have the lowest thermal conductivity. The Dulong-Petit law is obeyed at high temperature as expected. The phonon dispersion and density of states show that the d orbitals of Co and Nb are the significant contributors to the dispersions at both the acoustic and optical modes of the alloys.

Highlights

  • Introduction two main classes ofHeusler alloys; these are the full and halfHeusler alloys are a large family of alloys with properties that can be modified to suit technological applications in several areas of scientific and engineering research

  • In converged values for the smearing, lattice constant, k-point comparison, Nb and Sn have electronic configurations of (4d4 grid, and atomic positions were inputted for the electronic 5s1) and (5s2 5p2), respectively

  • At equilibrium tem- investigated the three possible configurations of the alloys to perature, the relevant information about the structural be- establish the equilibrium lattice constant and the most stable haviour of the alloys was extracted by fitting the result ob- structural state of the alloys

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Summary

Introduction

Introduction two main classes ofHeusler alloys; these are the full and halfHeusler alloys are a large family of alloys with properties that can be modified to suit technological applications in several areas of scientific and engineering research. Heusler alloys; these are the full and half. Heusler alloys are a large family of alloys with properties that can be modified to suit technological applications in several areas of scientific and engineering research. There are several variants arising from the two main classes [1,2,3,4,5]. Heusler first announced the full Heusler alloys in 1903 [6,7]; it has the X2YZ (2:1:1) stoichiometry and generally crystallises in the FCC phase and L21 structure. The half Heusler alloy, on the other hand, was discovered in 1983 by De Groot et al [8].

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