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超薄 FeSe 超导体中的巨大热电功率因子。

Giant thermoelectric power factor in ultrathin FeSe superconductor.

机构信息

RIKEN Center for Emergent Matter Science (CEMS), Wako, Saitama, 351-0198, Japan.

Institute for Materials Research, Tohoku University, Sendai, 980-8577, Japan.

出版信息

Nat Commun. 2019 Feb 18;10(1):825. doi: 10.1038/s41467-019-08784-z.

DOI:10.1038/s41467-019-08784-z
PMID:30778077
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6379375/
Abstract

The thermoelectric effect is attracting a renewed interest as a concept for energy harvesting technologies. Nanomaterials have been considered a key to realize efficient thermoelectric conversions owing to the low dimensional charge and phonon transports. In this regard, recently emerging two-dimensional materials could be promising candidates with novel thermoelectric functionalities. Here we report that FeSe ultrathin films, a high-T superconductor (T; superconducting transition temperature), exhibit superior thermoelectric responses. With decreasing thickness d, the electrical conductivity increases accompanying the emergence of high-T superconductivity; unexpectedly, the Seebeck coefficient α shows a concomitant increase as a result of the appearance of two-dimensional natures. When d is reduced down to ~1 nm, the thermoelectric power factor at 50 K and room temperature reach unprecedented values as high as 13,000 and 260 μW cm K, respectively. The large thermoelectric effect in high T superconductors indicates the high potential of two-dimensional layered materials towards multi-functionalization.

摘要

热电效应作为一种能源收集技术的概念,重新引起了人们的兴趣。由于低维电荷和声子输运,纳米材料被认为是实现高效热电转换的关键。在这方面,最近出现的二维材料可能是具有新颖热电功能的有前途的候选材料。在这里,我们报告说,FeSe 超薄薄膜(T;超导转变温度)表现出优异的热电响应。随着厚度 d 的减小,电导率增加,同时出现高温超导性;出乎意料的是,由于二维性质的出现,Seebeck 系数α也随之增加。当 d 减小到约 1nm 时,50K 和室温下的热电功率因子分别达到前所未有的 13000 和 260 μW cm K。高温超导体中的大热电效应表明二维层状材料在多功能化方面具有很高的潜力。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/b6607a500bd2/41467_2019_8784_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/c1198d172fab/41467_2019_8784_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/5e8e151cdbb8/41467_2019_8784_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/9f8d4a66d152/41467_2019_8784_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/b6607a500bd2/41467_2019_8784_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/c1198d172fab/41467_2019_8784_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/5e8e151cdbb8/41467_2019_8784_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/9f8d4a66d152/41467_2019_8784_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d5f9/6379375/b6607a500bd2/41467_2019_8784_Fig4_HTML.jpg

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