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Localised Ag(+) vibrations at the origin of ultralow thermal conductivity in layered thermoelectric AgCrSe(2)

In materials science, the substructure approach consists in imagining complex materials in which a particular property is associated with a distinct structural feature, so as to combine different chosen physical characteristics, which otherwise have little chance to coexist. Applied to thermoelectri...

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Detalles Bibliográficos
Autores principales: Damay, F., Petit, S., Rols, S., Braendlein, M., Daou, R., Elkaïm, E., Fauth, F., Gascoin, F., Martin, C., Maignan, A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4802330/
https://www.ncbi.nlm.nih.gov/pubmed/27000414
http://dx.doi.org/10.1038/srep23415
Descripción
Sumario:In materials science, the substructure approach consists in imagining complex materials in which a particular property is associated with a distinct structural feature, so as to combine different chosen physical characteristics, which otherwise have little chance to coexist. Applied to thermoelectric materials, it has been used to achieve simultaneously phonon-glass and electron-crystal properties. Mostly studied for its superionic conductivity, AgCrSe(2) is a naturally layered compound, which achieves very low thermal conductivity, ~0.4 W.K(−1).m(−1) at RT (room temperature), and is considered a promising thermoelectric. The Cr atoms of the [CrSe(2)](∞) layer bear a spin S = 3/2, which orders below T(N) = 55 K. Here we report low temperature inelastic neutron scattering experiments on AgCrSe(2), alongside the magnetic field evolution of its thermal and electrical transport. We observe a very low frequency mode at 3 meV, ascribed to large anharmonic displacements of the Ag(+) ions in the [Ag](∞) layer, and 2D magnetic fluctuations up to 3 T(N) in the chromium layer. The low thermal conductivity of AgCrSe(2) is attributed to acoustic phonon scattering by a regular lattice of Ag(+) oscillating in quasi-2D potential wells. These findings highlight a new way to achieve localised phonon modes in a perfectly crystalline solid.