Role of anharmonic strength and number of allowed three-phonon processes in lattice thermal conductivity of SnTe based compounds

The lattice heat transport properties of the thermoelectric (TE) material SnTe and the doped Sn7SbTe8 and Sn7BiTe8 are examined using Boltzmann transport theory supplemented with first-principle calculations. We illustrate the microscopic origin of the lattice thermal conductivity, κl of the materia...

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Published inJournal of physics. Condensed matter Vol. 33; no. 11; p. 115701
Main Authors Keshri, Sonu Prasad, Medhi, Amal
Format Journal Article
LanguageEnglish
Published England IOP Publishing 17.03.2021
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Summary:The lattice heat transport properties of the thermoelectric (TE) material SnTe and the doped Sn7SbTe8 and Sn7BiTe8 are examined using Boltzmann transport theory supplemented with first-principle calculations. We illustrate the microscopic origin of the lattice thermal conductivity, κl of the materials by calculating the mode Grüneisen parameters, phase space volume for three-phonon processes, the anharmonic scattering rates (SR), and the phonon group velocities. SnTe is found to be a low κl material with a value of ∼3 W mK−1 at room temperature in agreement with experiments. The phonon scatterings in pristine SnTe mainly originates in the strong anharmonicity of the material, as evidenced by the large values of its mode Grüneisen parameters. Doping with Sb or Bi reduces the anharmonic strength. For Sb doped Sn7SbTe8, it results in a drop in the SR and hence a higher κl value. However in the Bi doped Sn7BiTe8, the number of allowed three-phonon processes gets greatly enhanced which compensates for the reduction in anharmonicity. This coupled with lower phonon group velocities lowers the κl value for the Bi doped system below that of pristine SnTe. In nanowire structures, κl values for the doped systems get drastically reduced yielding an ultra-low value of 0.84 W mK−1 at 705 K for the Bi doped material for a nanowire of 10 nm diameter.
Bibliography:JPCM-117237.R2
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ISSN:0953-8984
1361-648X
DOI:10.1088/1361-648X/abd425