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Low-Thermal-Conductivity (MS)(1+x)(TiS(2))(2) (M = Pb, Bi, Sn) Misfit Layer Compounds for Bulk Thermoelectric Materials

A series of (MS)(1+x)(TiS(2))(2) (M = Pb, Bi, Sn) misfit layer compounds are proposed as bulk thermoelectric materials. They are composed of alternating rock-salt-type MS layers and paired trigonal anti-prismatic TiS(2) layers with a van der Waals gap. This naturally modulated structure shows low la...

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Detalles Bibliográficos
Autores principales: Wan, Chunlei, Wang, Yifeng, Wang, Ning, Koumoto, Kunihito
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Molecular Diversity Preservation International 2010
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5445838/
http://dx.doi.org/10.3390/ma3042606
Descripción
Sumario:A series of (MS)(1+x)(TiS(2))(2) (M = Pb, Bi, Sn) misfit layer compounds are proposed as bulk thermoelectric materials. They are composed of alternating rock-salt-type MS layers and paired trigonal anti-prismatic TiS(2) layers with a van der Waals gap. This naturally modulated structure shows low lattice thermal conductivity close to or even lower than the predicted minimum thermal conductivity. Measurement of sound velocities shows that the ultra-low thermal conductivity partially originates from the softening of the transverse modes of lattice wave due to weak interlayer bonding. Combined with a high power factor, the misfit layer compounds show a relatively high ZT value of 0.28~0.37 at 700 K.