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柔性混合无机-有机超晶格中的超高热电功率因子。

Ultrahigh thermoelectric power factor in flexible hybrid inorganic-organic superlattice.

机构信息

State Key Laboratory of New Ceramics and Fine Processing, School of Materials Science and Engineering, Tsinghua University, Beijing, 100084, China.

Toyota Physical and Chemical Research Institute, Nagakute, 480-1192, Japan.

出版信息

Nat Commun. 2017 Oct 18;8(1):1024. doi: 10.1038/s41467-017-01149-4.

DOI:10.1038/s41467-017-01149-4
PMID:29044102
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5647338/
Abstract

Hybrid inorganic-organic superlattice with an electron-transmitting but phonon-blocking structure has emerged as a promising flexible thin film thermoelectric material. However, the substantial challenge in optimizing carrier concentration without disrupting the superlattice structure prevents further improvement of the thermoelectric performance. Here we demonstrate a strategy for carrier optimization in a hybrid inorganic-organic superlattice of TiS[tetrabutylammonium] [hexylammonium] , where the organic layers are composed of a random mixture of tetrabutylammonium and hexylammonium molecules. By vacuum heating the hybrid materials at an intermediate temperature, the hexylammonium molecules with a lower boiling point are selectively de-intercalated, which reduces the electron density due to the requirement of electroneutrality. The tetrabutylammonium molecules with a higher boiling point remain to support and stabilize the superlattice structure. The carrier concentration can thus be effectively reduced, resulting in a remarkably high power factor of 904 µW m K at 300 K for flexible thermoelectrics, approaching the values achieved in conventional inorganic semiconductors.

摘要

具有电子输运但声子阻断结构的混合无机-有机超晶格作为一种很有前途的柔性薄膜热电材料而出现。然而,在不破坏超晶格结构的情况下优化载流子浓度的巨大挑战,阻碍了热电性能的进一步提高。在这里,我们展示了一种在 TiS[四丁基铵][己基铵]的混合无机-有机超晶格中进行载流子优化的策略,其中有机层由四丁基铵和己基铵分子的随机混合物组成。通过在中间温度下对混合材料进行真空加热,沸点较低的己基铵分子被选择性地脱插,由于电中性的要求,电子密度降低。沸点较高的四丁基铵分子保持不变,以支撑和稳定超晶格结构。因此,载流子浓度可以有效地降低,从而在 300 K 时为柔性热电材料实现高达 904 µW m K 的显著高功率因子,接近传统无机半导体的数值。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/4495280ac31d/41467_2017_1149_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/cb69dc062e88/41467_2017_1149_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/e37c7b7adf4a/41467_2017_1149_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/2a2d06459ea2/41467_2017_1149_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/7ae6b6bc5564/41467_2017_1149_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/4495280ac31d/41467_2017_1149_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/cb69dc062e88/41467_2017_1149_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/e37c7b7adf4a/41467_2017_1149_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/2a2d06459ea2/41467_2017_1149_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/7ae6b6bc5564/41467_2017_1149_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5ae/5647338/4495280ac31d/41467_2017_1149_Fig5_HTML.jpg

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