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Tuning Transport Properties in Thermoelectric Nanocomposites through Inorganic Ligands and Heterostructured Building Blocks

[Image: see text] Methodologies that involve the use of nanoparticles as “artificial atoms” to rationally build materials in a bottom-up fashion are particularly well-suited to control the matter at the nanoscale. Colloidal synthetic routes allow for an exquisite control over such “artificial atoms”...

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Detalles Bibliográficos
Autores principales: Ibáñez, Maria, Genç, Aziz, Hasler, Roger, Liu, Yu, Dobrozhan, Oleksandr, Nazarenko, Olga, Mata, María de la, Arbiol, Jordi, Cabot, Andreu, Kovalenko, Maksym V.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2019
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6595432/
https://www.ncbi.nlm.nih.gov/pubmed/31185159
http://dx.doi.org/10.1021/acsnano.9b00346
Descripción
Sumario:[Image: see text] Methodologies that involve the use of nanoparticles as “artificial atoms” to rationally build materials in a bottom-up fashion are particularly well-suited to control the matter at the nanoscale. Colloidal synthetic routes allow for an exquisite control over such “artificial atoms” in terms of size, shape, and crystal phase as well as core and surface compositions. We present here a bottom-up approach to produce Pb–Ag–K–S–Te nanocomposites, which is a highly promising system for thermoelectric energy conversion. First, we developed a high-yield and scalable colloidal synthesis route to uniform lead sulfide (PbS) nanorods, whose tips are made of silver sulfide (Ag(2)S). We then took advantage of the large surface-to-volume ratio to introduce a p-type dopant (K) by replacing native organic ligands with K(2)Te. Upon thermal consolidation, K(2)Te-surface modified PbS–Ag(2)S nanorods yield p-type doped nanocomposites with PbTe and PbS as major phases and Ag(2)S and Ag(2)Te as embedded nanoinclusions. Thermoelectric characterization of such consolidated nanosolids showed a high thermoelectric figure-of-merit of 1 at 620 K.