Anomalous thermoelectricity of pure ZnO from 3D continuous ultrathin nanoshell structures

ZnO is a potential thermoelectric material because of its non-toxicity, high thermal stability, and relatively high Seebeck coefficient (S) of metal oxides. However, the extremely low figure of merit (zT), which comes from a high thermal conductivity (κ) over 40 W m K , limits the thermoelectric app...

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Published inNanoscale Vol. 10; no. 6; pp. 3046 - 3052
Main Authors Kim, Kisun, Park, Junyong, Hong, Seokkyoon, Park, Sun Hwa, Jeon, Seong Gi, Ahn, Changui, Song, Jae Yong, Jeon, Seokwoo
Format Journal Article
LanguageEnglish
Published England Royal Society of Chemistry 01.01.2018
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Summary:ZnO is a potential thermoelectric material because of its non-toxicity, high thermal stability, and relatively high Seebeck coefficient (S) of metal oxides. However, the extremely low figure of merit (zT), which comes from a high thermal conductivity (κ) over 40 W m K , limits the thermoelectric application of ZnO. In particular, below 500 K, ZnO exhibits a nearly negligible zT (<10 ), unless a dopant is incorporated into the crystal structure. Here, we propose a new strategy for achieving a reduced κ and a correspondingly increased zT of pure ZnO over a wide temperature range from 333 K to 723 K by forming an ∼72 nm thick, 3D continuous ultrathin nanoshell structure. The suppressed κ of the 3D ZnO film is ∼3.6 W m K at 333 K, which is ∼38 times lower than that of the blanket ZnO film (3.2 μm thick), which was set as a reference. The experimental zT of the 3D ZnO film is ∼0.017 at 333 K, which is the highest value among pure ZnO reported to date and is estimated to increase by ∼0.072 at 693 K according to the Debye-Callaway approach. Large-area (∼1 in ) fabrication of the 3D ZnO film with high structural uniformity allows the realization of an integrated thermoelectric device, which generates ∼60 mV at a temperature difference of 40 K along the in-plane direction.
ISSN:2040-3364
2040-3372
DOI:10.1039/c7nr08167g