Abstract

The surface free energies of seven different facets of tungsten (W) are obtained up to the melting point with full account of all the relevant thermal excitations; in particular, thermal atomic vibrations, electronic excitations, and their mutual coupling. The latter is done using ab initio molecular dynamics simulations coupled with the thermodynamic integration technique. In this way, the calculations contain almost no error but the one related to the used exchange-correlation functional, which makes the results truly first principles. The obtained results are compared with previous quasiharmonic calculations for the surface free energies of W and experimental data. The anharmonic contribution is, as expected, important for open surfaces at high temperatures, which leads to a temperature dependence of the surface energy anisotropy. The calculated Wulff shapes and surface energies are in excellent agreement with experimental data close to the melting point, where the crystalline structure of the surface layers is destroyed by a dramatic mobility of the atoms there.

Highlights

  • Surface energies of solids can only be measured at temperatures close to the melting point, and high temperature data from calculations are the only way to connect calculations to experiments [1]

  • Such calculations are in general a nontrivial task due to the necessity to account for all the relevant thermal excitations and their coupling

  • The most important contribution from the thermal lattice vibrations can be accounted for within the quasiharmonic approximation (QHA), which has been previously used in a number of ab initio surface energy calculations at finite temperature [2,3,4,5,6]

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Summary

Introduction

Surface energies of solids can only be measured at temperatures close to the melting point, and high temperature data from calculations are the only way to connect calculations to experiments [1]. Such calculations are in general a nontrivial task due to the necessity to account for all the relevant thermal excitations and their coupling. While the QHA is reasonably accurate for most defect-free bulk systems, it misses anharmonic contributions. These contributions can be quite substantial, especially at high temperatures in systems with open defects. A strong anharmonic contribution has been obtained for Al surfaces in modeling with classical potentials [10]

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