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Volume 29 (1–4) 2023, 57–64

Density Functional Formalism as a Description of the Elastic Behavior of a Hard-Sphere Crystal

Pieprzyk S. 1*, Brańka A.C. 1†, Heyes D.M. 2

1 Institute of Molecular Physics
Polish Academy of Sciences
M. Smoluchowskiego 17, 60-179 Poznań, Poland
∗E-mail: slawomir.pieprzyk@ifmpan.poznan.pl
†E-mail: branka@ifmpan.poznan.pl

2 Royal Holloway, University of London
Department of Physics
Egham, Surrey TW20 0EX, United Kingdom
E-mail: david.heyes@rhul.ac.uk

Received:

Received: 13 November 2023; in final form: 20 November 2023; accepted: 21 November 2023; published online: 9 December 2023

DOI:   10.12921/cmst.2023.0000027

Abstract:

The density functional method of Jarić and Mohanty [Phys. Rev. B 37, 4441 (1988)] for calculating the elastic moduli of crystalline solids is considered here from the perspective of some new findings. The very slow convergence of the reciprocal lattice vector summations and presence of the three body term in the method’s computational scheme identified in [J. Chem. Phys. 118, 6594 (2003)] is confirmed and discussed. The sensitivity of the results to the scheme parameters, such as the width of the Gaussian density profiles and the Percus-Yevick approximation used for the direct correlation function is explored. The calculations are for a hard-sphere crystal but most conclusions can be applicable to model crystalline solids in general.

Key words:

density functional theory, elastic moduli tensor, hard spheres

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