Density Functional Study of the L1_0 - alpha-IrV Transition in IrV and RhV

TL;DR

This study uses first-principles calculations to investigate the phase transition between alpha-IrV and L1_0 structures in IrV and RhV, revealing it is likely a weakly first-order transition driven by electronic density of states changes.

Contribution

It provides a detailed computational analysis showing the transition is not second order, involving stable phonons at the R point, and identifies the transition as likely weakly first order.

Findings

Transition driven by electronic density of states at Fermi level.

All phonons at R point are stable, contrary to previous assumptions.

Transition involves volume and energy discontinuities.

Abstract

Both IrV and RhV crystallize in the alpha-IrV structure, with a transition to the higher symmetry L1_0 structure at high temperature, or with the addition of excess Ir or Rh. Here we present evidence that this transition is driven by the lowering of the electronic density of states at the Fermi level of the alpha-IrV structure. The transition has long been thought to be second order, with a simple doubling of the L1_0 unit cell due to an unstable phonon at the R point (0 1/2 1/2). We use first-principles calculations to show that all phonons at the R point are, in fact, stable, but do find a region of reciprocal space where the L1_0 structure has unstable (imaginary frequency) phonons. We use the frozen phonon method to examine two of these modes, relaxing the structures associated with the unstable phonon modes to obtain new structures which are lower in energy than L1_0 but still above alpha-IrV. We examine the phonon spectra of these structures as well, looking for instabilities, and find further instabilities, and more relaxed structures, all of which have energies above the alpha-IrV phase. In addition, we find that all of the relaxed structures, stable and unstable, have a density comparable to the L1_0 phase (and less than the alpha-IrV phase), so that any transition from one of these structures to the ground state will have a volume change as well as an energy discontinuity. We conclude that the transition from L1_0 to alpha-IrV is probably weakly first order.