Xia Yi, Pal Koushik, He Jiangang, Ozoliņš Vidvuds, Wolverton Chris
Department of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, USA.
Department of Applied Physics, Yale University, New Haven, Connecticut 06511, USA.
Phys Rev Lett. 2020 Feb 14;124(6):065901. doi: 10.1103/PhysRevLett.124.065901.
We investigate the microscopic mechanisms of ultralow lattice thermal conductivity (κ_{l}) in Tl_{3}VSe_{4} by combining a first principles density functional theory based framework of anharmonic lattice dynamics with the Peierls-Boltzmann transport equation for phonons. We include contributions of the three- and four-phonon scattering processes to the phonon lifetimes as well as the temperature dependent anharmonic renormalization of phonon energies arising from an unusually strong quartic anharmonicity in Tl_{3}VSe_{4}. In contrast to a recent report by Mukhopadhyay et al. [Science 360, 1455 (2018)SCIEAS0036-807510.1126/science.aar8072] which suggested that a significant contribution to κ_{l} arises from random walks among uncorrelated oscillators, we show that particlelike propagation of phonon excitations can successfully explain the experimentally observed ultralow κ_{l}. Our findings are further supported by explicit calculations of the off-diagonal terms of the heat current operator, which are found to be small and indicate that wavelike tunneling of heat carrying vibrations is of minor importance. Our results (i) resolve the discrepancy between the theoretical and experimental κ_{l}, (ii) offer new insights into the minimum κ_{l} achievable in Tl_{3}VSe_{4}, and (iii) highlight the importance of high order anharmonicity in low-κ_{l} systems. The methodology demonstrated here may be used to resolve the discrepancies between the experimentally measured and the theoretically calculated κ_{l} in skutterides and perovskites, as well as to understand the glasslike κ_{l} in complex crystals with strong anharmonicity, leading towards the goal of rational design of new materials.
我们通过将基于第一性原理密度泛函理论的非谐晶格动力学框架与声子的派尔斯 - 玻尔兹曼输运方程相结合,研究了Tl₃VSe₄中超低晶格热导率(κₗ)的微观机制。我们考虑了三声子和四声子散射过程对声子寿命的贡献,以及由于Tl₃VSe₄中异常强的四次非谐性引起的声子能量的温度依赖性非谐重整化。与Mukhopadhyay等人最近的一篇报告[《科学》360, 1455 (2018)SCIEAS0036 - 807510.1126 / science.aar8072]不同,该报告认为κₗ的显著贡献来自不相关振子之间的随机游走,我们表明声子激发的类粒子传播能够成功解释实验观测到的超低κₗ。热流算符非对角项的显式计算进一步支持了我们的发现,这些非对角项被发现很小,表明携带热量振动的波状隧穿不太重要。我们的结果(i)解决了理论和实验κₗ之间的差异,(ii)为Tl₃VSe₄中可实现的最低κₗ提供了新的见解,(iii)强调了高阶非谐性在低κₗ系统中的重要性。这里展示的方法可用于解决方钴矿和钙钛矿中实验测量的κₗ与理论计算的κₗ之间的差异,以及理解具有强非谐性的复杂晶体中的玻璃状κₗ,朝着合理设计新材料的目标迈进。