# New two-dimensional phase of tin chalcogenides: candidates for high-performance thermoelectric materials

## TL;DR

This study predicts a new 2D hexagonal phase of tin chalcogenides with high thermoelectric efficiency, using computational methods to identify stable structures and evaluate their thermoelectric properties.

## Contribution

The paper introduces a novel 2D hexagonal phase of SnX (X=Te, Se, S) discovered via evolutionary algorithms, demonstrating high thermoelectric performance.

## Key findings

- $eta'$-SnTe is the most stable 2D phase among SnTe structures.
- High ZT values (up to 3.81) achieved at 900K for $eta'$-SnX.
- High thermoelectric performance attributed to quantum confinement, band convergence, and low thermal conductivity.

## Abstract

Tin-chalcogenides SnX (X = Te, Se and S) have been arousing research interest due to their thermoelectric physical properties. The two-dimensional (2D) counterparts, which are expected to enhance the property, nevertheless, have not been fully explored because of many possible structures. Generating variable composition of 2D Sn$_{1-x}$X$_{x}$ systems (X = Te, Se and S) has been performed using global searching method based on evolutionary algorithm combining with density functional calculations. A new hexagonal phase named by $\beta'$-SnX is found by Universal Structure Predictor Evolutionary Xtallography (USPEX), and the structural stability has been further checked by phonon dispersion calculation and the elasticity criteria. The $\beta'$-SnTe is the most stable among all possible 2D phases of SnTe including those experimentally available phases. Further, $\beta'$ phases of SnSe and SnS are also found energetically close to the most stable phases. High thermoelectronic (TE) performance has been achieved in the $\beta'$-SnX phases, which have dimensionless figure of merit (ZT) as high as $\sim$0.96 to 3.81 for SnTe, $\sim$0.93 to 2.51 for SnSe and $\sim$1.19 to 3.18 for SnS at temperature ranging from 300 K to 900 K with practically attainable carrier concentration of 5$\times$10$^{12}$ cm$^{-2}$. The high TE performance is resulted from a high power factor which is attributed to the quantum confinement of 2D materials and the band convergence near Fermi level, as well as low thermal conductivity mainly from both low elastic constants due to weak inter-Sn bonding strength and strong lattice anharmonicity.