Thermal conductivity is a key materials parameter that is important in combination with other properties for important applications including electronics, thermal barriers and a variety of energy technologies. There are established trends that are useful in finding materials with desirable thermal conductivity. For example, stable stiff lattices typically yield high thermal conductivity, while materials near instabilities have low thermal conductivity. Rattling is widely applied approach for lowering thermal conductivity and is understood as the incorporation of loosely bound ions in a semiconducting framework. It is manifested in low frequency flat optical phonon branches that cross the acoustic branches. We investigate LaRhTe using global optimization crystal structure determination, anharmonic lattice dynamics, and first principles based characterization of bonding. There are two low energy phases, a hexagonal metallic phase and a cubic semiconducting phase. This cubic phase is predicted to be a low thermal conductivity (1.61 W m−1K−1 at 300 K) semiconductor. We elucidate the origins of its low thermal conductivity finding that strong anharmonic phonon scattering, induced by weak bonding of Rh within the cage-like LaTe network, is important. The Rh atoms contribute to low-frequency phonons, while the La-Te system dominates the high-frequency optical phonon branches. This is unexpected based on the chemical characteristics of Rh chalcogenides and the known thermoelectric behavior of La-Te binary phases. It arises due to the structural constraints in the cubic half-Heusler phase leading to a generalized rattling behavior involving Rh. These results show that the rattling concept is more general than usually assumed and can be operative even without the characteristic rattler induced flat optical branches anticrossing the acoustic branches that are often discussed in the context of low thermal conductivity thermoelectrics.
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