Lattice thermal conductivity of CsSnBr3/Cs2SnBr6 interface from ab initio based neuroevolution potential simulations
Jinge Han1, Jun Tang1, Hehuan Bai1
1Key Laboratory of Optoelectronic Technology and Systems (Ministry of Education), College of Optoelectronic Engineering, Chongqing University, Chongqing 400044, China.
The Journal of Chemical Physics
|July 25, 2025
Summary
Researchers achieved ultralow thermal conductivity in CsSnBr3/Cs2SnBr6 interfaces using atomic molecular dynamics. This breakthrough in phonon engineering is key for developing advanced energy conversion devices.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Nanotechnology
Background:
- Engineering interface phonons is critical for developing materials with extremely low thermal conductivity.
- Such materials are essential components for efficient energy conversion devices.
Purpose of the Study:
- To report ultralow lattice thermal conductivity at the CsSnBr3/Cs2SnBr6 interface.
- To investigate the mechanisms behind this low thermal transport.
Main Methods:
- Large-scale atomic molecular dynamics (MD) simulations.
- Ab initio density functional theory (DFT) calculations to derive accurate neuroevolution potentials.
- Analysis of phonon scattering, localization, and anharmonicity.
Main Results:
- Achieved an ultralow lattice thermal conductivity of 0.173 W m−1 K−1 at the CsSnBr3/Cs2SnBr6 interface.
- Observed enhanced anharmonicity and significant phonon scattering/localization.
- Identified a strong mixed phonon liquid character and nonlinear interface density-dependent thermal conductivity.
Conclusions:
- The CsSnBr3/Cs2SnBr6 interface exhibits exceptional phononic properties for thermal management.
- Findings provide insights for designing crystalline anisotropic thermoelectric materials.
- Phonon engineering at interfaces is a viable strategy for advanced thermoelectric applications.
Related Concept Videos
Trends in Lattice Energy: Ion Size and Charge
24.3K
An ionic compound is stable because of the electrostatic attraction between its positive and negative ions. The lattice energy of a compound is a measure of the strength of this attraction. The lattice energy (ΔHlattice) of an ionic compound is defined as the energy required to separate one mole of the solid into its component gaseous ions. For the ionic solid sodium chloride, the lattice energy is the enthalpy change of the process:
24.3K
The Born-Haber Cycle
22.3K
Lattice Energy
22.3K
Network Covalent Solids
14.6K
Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
14.6K
Van der Waals Interactions
66.6K
Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.
66.6K
Lattice Centering and Coordination Number
9.9K
The structure of a crystalline solid, whether a metal or not, is best described by considering its simplest repeating unit, which is referred to as its unit cell. The unit cell consists of lattice points that represent the locations of atoms or ions. The entire structure then consists of this unit cell repeating in three dimensions. The three different types of unit cells present in the cubic lattice are illustrated in Figure 1.
Types of Unit Cells
Imagine taking a large number of identical...
Types of Unit Cells
Imagine taking a large number of identical...
9.9K
Molecular and Ionic Solids
17.6K
Crystalline solids are divided into four types: molecular, ionic, metallic, and covalent network based on the type of constituent units and their interparticle interactions.
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
17.6K


