Pressure-induced toroidal order in molecular Sn$_2$P$_2$S$_6$ ferroelectrics

TL;DR

This study uses ab initio molecular dynamics and evolutionary algorithms to explore pressure-induced structural transformations in Sn$_2$P$_2$S$_6$, revealing the emergence of toroidal order and potential links to superconductivity.

Contribution

It provides new insights into pressure-induced phase transformations and the formation of toroidal order in Sn$_2$P$_2$S$_6$ using advanced computational methods.

Findings

Pressure breaks P-P bonds, altering molecular structure.

Toroidally ordered local dipoles appear in the centrosymmetric phase.

Structural models align with experimental volume dependence data.

Abstract

For the Sn$_2$P$_2$S$_6$ crystalline compound with a rich temperature--pressure phase diagram that contains the ferroelectric phase, semiconductor-to-metal transition, and superconductive state, \mbox{\textit{ab initio}} molecular dynamics calculations were performed on a single unit cell and on a superstructure using an evolutionary algorithm in combination with density functional theory calculations to study structural transformations resulting from rearrangements in chemical bonds under pressure. The structure models of the pressure-induced lowest energy phases in the molecular Sn$_2$P$_2$S$_6$ crystal demonstrate the possibility of space-arranged chains or rings of P$_2$S$_6$ molecules. Pressure can break P-P bonds of P$_2$S$_6$ molecules, causing one of the phosphorous atoms to displace into the sulfur-formed octahedron and providing another phosphorous atom into an octahedral coordination with two tin atoms and four sulfur atoms. The results of the modeling correlate with the gradual rise of deviation of the pressure dependence of the unit cell volume of the Sn$_2$P$_2$S$_6$ structure, as determined by X-ray diffraction experiments, from the dependence calculated with the Birch-Murnaghan equation of state. It also reveals toroidally ordered local dipoles in the centrosymmetric phase, which may be related to the previously observed superconductivity in the high-pressure metallic phase of Sn$_2$P$_2$S$_6$.