Dramatically reduced lattice thermal conductivity of Mg 2 Si thermoelectric material from nanotwinning, Acta Materialia, https://doi.
Abstract:Tuning phonon transport to reduce the lattice thermal conductivity (κ L ) is crucial for advancing thermoelectrics (TEs). Traditional strategies on κ L reduction focus on introducing scattering sources such as point defects, dislocations, and grain boundaries, that may degrade the electrical conductivity and Seebeck coefficient. We suggest here, a novel twin boundary (TB) strategy that can decrease the κ L of Mg 2 Si by ~90%, but which may not degrade the electrical properties significantly. We validate this suggestion using density functional theory (DFT). We attribute the mechanism of TB induced κ L reduction to (i) the lower phonon velocities and larger Grüneisen parameter, (ii) "rattling" of the Mg−Mg pair induced soft acoustic and optical modes, (iii) shorter phonon lifetime and higher phonon scattering rate. We predict that the size of nanotwinned structure should be controlled between 3 nm and 100 nm in the Mg 2 Si matrix for the most effective κ L reduction. These results should be applicable for other TE or non TE energy materials with desired low thermal conductivity, suggesting rational designs of high-performance Mg 2 Si TE materials with low κ L for the energy conversion applications. Functional Theory 0.4 W m −1 K −1 and a zT of 1.5 at 1000 K [21]. In SnSe single crystals, The lattice anharmonicity leads to an exceptionally low κ L of 0.23 ± 0.03 W m −1 K −1 and an unprecedented zT of 2.6 ± 0.03 at 923 K [22,23]. In such TE materials as MgAgSb [24], Ag 5-δ Te 3 [25], and Ag 8 SnSe 6 [26], the complex crystal structure or weak chemical bonds leads to low heat capacity or low speed of sound, well explaining the low intrinsic κ L of < 0.5 W m −1 K [24-26]. Introducing phonon scattering sources such as point defects [27-29], dislocations [30-32], grain boundaries [33-35], can effectively shorten phonon relaxation time, giving rise to reduction in κ L . Multiple fillers inCoSb 3 can achieve broad-frequency phonon scattering, reducing κ L to the glass limit value of 0.2 W m −1 K −1 , and leading to an extremely high zT of 1.7 at 850 K [29]. Full-spectrum phonon scattering, which was achieved through grain boundary, dense dislocation arrays, and point defect,