Additional phonon scattering channels provided by one-dimensional heavy double-chain rattlers in quasi-one-dimensional perovskite
Phys. Rev. B 113, 184311 – Published 11 May, 2026
DOI: https://doi.org/10.1103/873p-hdjm
Abstract
Host-guest crystalline materials with strong anharmonicity exhibiting long-range order and local disorder offer a paradigm for ideal thermoelectric model known as the “phonon-glass electron-crystal” (PGEC), which ensures efficient electrical conduction characteristic of crystals while suppressing thermal transport in a glasslike manner. It is widely accepted that guest atoms introduce low-frequency low-lying optical phonons (referred to as rattling modes), which intensely scatter the acoustic phonons, thereby drastically reducing lattice thermal conductivity (). In quasi-one-dimensional (Q-1D) thermoelectrics, this mechanism is conceptualized as covalent 1D chains forming the host framework, with isolated interchain ions acting as charge-balancing rattlers to further dampen . However, our first-principles studies of the Q-1D perovskite reveal that the covalent 1D chains serving as host frames also produce low-lying optical phonons, which introduce additional three-phonon scattering channels. Utilizing self-consistent phonon theory and Wigner transport formalism, we capture phonon frequency renormalization and wavelike coherent scattering. This approach uncovers an ultralow with weak temperature dependence, consistent with the results from homogeneous nonequilibrium molecular dynamics. Furthermore, based on a low-order expansion of electron-phonon coupling, we estimate a thermoelectric figure of merit up to 0.53 (0.92) at 300 (425) K for . Notably, we identify the low-lying optical branches originating from the antiparallel sliding of the host 1D chains, offering additional phonon scattering channels for damping phonon transport. These findings offer new microscopic insights into Q-1D thermoelectric transport and provide a viable material platform and a design scheme to explore PGEC behavior in anisotropic systems.