Thermoelectric properties of 3D topological insulator: Direct observation of topological surface and its gap opened states

Thermoelectric properties of 3D topological insulator: Direct observation of topological surface and its gap opened states
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DOI:
10.1103/physrevmaterials.1.054202
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发表时间:
2017-03
期刊:
arXiv: Materials Science
影响因子:
--
通讯作者:
S. Y. Matsushita;K. K. Huynh-K.;H. Yoshino;N. Tu;Y. Tanabe;K. Tanigaki
S. Y. Matsushita;K. K. Huynh-K.;H. Yoshino;N. Tu;Y. Tanabe;K. Tanigaki
中科院分区:
其他
文献类型:
--
作者:
S. Y. Matsushita;K. K. Huynh-K.;H. Yoshino;N. Tu;Y. Tanabe;K. Tanigaki

文献摘要

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通过采用超薄外延生长的单晶Bi $_{2-x}$ Sb $_x$ TE $_{3-y}$ Se $_y$薄膜,我们报道了三维拓扑绝缘体(3D-TIs)中拓扑表面狄拉克态(TSDS)的热电(TE)性质。通过电输运,我们成功地观察到了金属TSDS (m-TSDS)和开隙半导体拓扑态(g-TSDS)这两个本征非简单表面拓扑态,并精确地确定了重要的TE参数(电导率(${\sigma}$)、导热系数(${\kappa}$)和热功率($S$))。纯m-TSDS得到$S$ =-44 {\mu} VK $^{-1}$,比常规金属高一个数量级,g-TSDS得到-212 {\mu} VK $^{-1}$。结果清楚地表明,最常用于常规分析的恒定松弛时间(${\tau}$)框架下的半经典玻尔兹曼输移方程(SBTE)在3d - ti中是不成立的,而超越玻恩近似的强能量依赖的松弛时间${\tau}(E)$对于进行内在解释是必不可少的。虽然${\sigma}$在m-TSDS上受到保护,但${\kappa}$受到拓扑表面无序的极大影响,使得拓扑保护下的电子传导和声子输运的效果不同。
We report thermoelectric (TE) properties of topological surface Dirac states (TSDS) in three-dimensional topological insulators (3D-TIs) purely isolated from the bulk by employing single crystal Bi$_{2-x}$Sb$_x$Te$_{3-y}$Se$_y$ films epitaxially grown in the ultrathin limit. Two intrinsic nontrivial topological surface states, a metallic TSDS (m-TSDS) and a gap-opened semiconducting topological state (g-TSDS), are successfully observed by electrical transport, and important TE parameters (electrical conductivity (${\sigma}$), thermal conductivity (${\kappa}$), and thermopower ($S$)) are accurately determined. Pure m-TSDS gives $S$=-44 {\mu}VK$^{-1}$, which is an order of magnitude higher than those of the conventional metals and the value is enhanced to -212 {\mu}VK$^{-1}$ for g-TSDS. It is clearly shown that the semi-classical Boltzmann transport equation (SBTE) in the framework of constant relaxation time (${\tau}$) most frequently used for conventional analysis cannot be valid in 3D-TIs and strong energy dependent relaxation time ${\tau}(E)$ beyond the Born approximation is essential for making intrinsic interpretations. Although ${\sigma}$ is protected on the m-TSDS, ${\kappa}$ is greatly influenced by the disorder on the topological surface, giving a dissimilar effect between topologically protected electronic conduction and phonon transport.