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The EXP pair-potential system. III. Thermodynamic phase diagram.

Authors :
Pedersen, Ulf R.
Bacher, Andreas K.
Schrøder, Thomas B.
Dyre, Jeppe C.
Source :
Journal of Chemical Physics. 2019, Vol. 150 Issue 17, pN.PAG-N.PAG. 9p. 1 Diagram, 2 Charts, 8 Graphs.
Publication Year :
2019

Abstract

This paper determines the thermodynamic phase diagram of the EXP system of particles interacting by the purely repulsive exponential pair potential. The solid phase is face-centered cubic (fcc) at low densities and pressures. At higher densities and pressures, the solid phase is body-centered cubic (bcc) with a re-entrant liquid phase at the highest pressures simulated. The investigation first identifies the phase diagram at zero temperature at which the following four crystal structures are considered: fcc, bcc, hexagonal close packed, and cubic diamond. There is a T = 0 phase transition at pressure 2.651 × 10−3 with the thermodynamically stable structure being fcc below and bcc above this pressure. The densities of the two crystal structures at the phase transition are 1.7469 × 10−2 (fcc) and 1.7471 × 10−2 (bcc). At finite temperatures, the fcc–bcc, fcc-liquid, and bcc-liquid coexistence lines are determined by numerical integration of the Clausius–Clapeyron equation and validated by interface-pinning simulations at selected state points. The bcc-fcc phase transition is a weak first-order transition. The liquid-fcc–bcc triple point, which is determined by the interface-pinning method, has temperature 5.9 × 10−5 and pressure 2.5 × 10−6; the triple-point densities are 1.556 × 10−3 (liquid), 1.583 × 10−3 (bcc), and 1.587 × 10−3 (fcc). [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00219606
Volume :
150
Issue :
17
Database :
Academic Search Index
Journal :
Journal of Chemical Physics
Publication Type :
Academic Journal
Accession number :
136340907
Full Text :
https://doi.org/10.1063/1.5094395