Lawrence Berkeley National Laboratory

Charge and thermal transport in a crystal is carried by free electrons and phonons (quantized lattice vibration), the two most fundamental quasiparticles. Above the Debye temperature of the crystal, phonon-mediated thermal conductivity (κ _L) is typically limited by mutual scattering of phonons, which results in κ _L decreasing with inverse temperature, whereas free electrons play a negligible role in κ _L. Here, an unusual case in charge-density-wave tantalum disulfide (1T-TaS₂) is reported, in which κ _L is limited instead by phonon scattering with free electrons, resulting in a temperature-independent κ _L. In this system, the conventional phonon-phonon scattering is alleviated by its uniquely structured phonon dispersions, while unusually strong electron-phonon (e-ph) coupling arises from its Fermi surface strongly nested at wavevectors in which phonons exhibit Kohn anomalies. The unusual temperature dependence of thermal conduction is found as a consequence of these effects. The finding reveals new physics of thermal conduction, offers a unique platform to probe e-ph interactions, and provides potential ways to control heat flow in materials with free charge carriers. The temperature-independent thermal conductivity may also find thermal management application as a special thermal interface material between two systems when the heat conduction between them needs to be maintained at a constant level.