Answers are grounded in this paper and cite their sources.
We report that K 2 Bi 8 Se 13 exhibits multiple conduction bands that lie close in energy and can be activated through doping, leading to a highly enhanced Seebeck coefficient and a high power factor with elevated temperature. Meanwhile, the large unit cell, complex low symmetry crystal structure, and nondirectional bonding lead to the very low lattice thermal conductivity of K 2 Bi 8 Se 13, ranging between 0.42 and 0.20 W m –1 K –1 in the temperature interval 300–873 K. Experimentally, we further support the low thermal conductivity of K 2 Bi 8 Se 13 using phonon velocity measurements; the results show a low average phonon velocity (1605 ms –1 ), small Young’s modulus (37.1 GPa), large Grüneisen parameter (1.71), and low Debye temperature (154 K). A detailed investigation of the microstructure and defects was carried out using electron diffraction and transmission microscopy which reveal the presence of a K 2.5 Bi 8.5 Se 14 minor phase intergrown along the side of the K 2 Bi 8 Se 13 phase. The combination of enhanced power factor and low thermal conductivity results in a high ZT value of ∼1.3 at 873 K in electron doped K 2 Bi 8 Se 13 material.
No takes yet. Share an insight, caveat, or question.
Pei et al. (2016) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: