Abstract

The Fe–Ni–Si system is potentially a very important component of terrestrial planetary cores. However, at present, even the behaviour of the FeSi and NiSi end members is poorly understood, especially at low to moderate pressures—the data for FeSi are contradictory and NiSi has been little studied. For FeSi, there is general agreement that there is a phase transition from the ε-FeSi to the CsCl structure with increasing pressure, but, in experiments, there is disagreement as to the position and slope of the phase boundary and the range of coexistence of the two phases. In this paper we have used ab initio lattice dynamics calculations to determine the phase boundary between the ε-FeSi and CsCl structures as a function of pressure and temperature in both FeSi and NiSi. For FeSi, we find that the transition pressure at zero Kelvin is ~11 GPa and that the boundary between the ε-FeSi and CsCl phases varies little with temperature, having a slight negative Clapeyron slope, going from ~11 GPa at 300 K to ~3 GPa at 2000 K. For NiSi, there is much greater variation of the transition pressure with temperature, with a much shallower negative Clapeyron slope, going from ~156 GPa at 300 K to ~94 GPa at 2000 K.

Highlights

  • It is widely accepted from cosmochemical and geophysical arguments that the Earth’s core, as well as the cores of the terrestrial planets, is comprised of mainly iron alloyed with nickel and a small proportion of light element(s)

  • Corresponding experimental values for NiSi are extremely limited as both of these structures are only found at high pressures

  • For CsCl-structured NiSi it is difficult to make a meaningful comparison with experiments, since these give values ranging from ~150 < K0 < 240

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Summary

Introduction

It is widely accepted from cosmochemical and geophysical arguments that the Earth’s core, as well as the cores of the terrestrial planets, is comprised of mainly iron alloyed with nickel and a small proportion of light element(s). Both experiments and calculations find only two stable structures in the FeSi system, the ε-FeSi phase and the CsCl phase (Vočadlo et al 1999; Caracas and Wentzcovitch 2004; Lord et al 2010; Fischer et al 2013; Geballe and Jeanloz 2014).

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