掺杂剂
材料科学
凝聚态物理
兴奋剂
费米能级
原子轨道
带隙
电子结构
价(化学)
密度泛函理论
布里渊区
热电材料
态密度
热电效应
光电子学
计算化学
化学
物理
量子力学
电子
作者
Guodong Tang,Yuqi Liu,Jing Wang,Yongsheng Zhang,Pengfei Nan,Pan Ying,Yaru Gong,Xuemei Zhang,Binghui Ge,Nan Lin,Xuefei Miao,Kun Song,Carl‐Friedrich Schön,Matteo Cagnoni,Dasol Kim,Yuan Yu,Matthias Wuttig
标识
DOI:10.1038/s41467-024-53599-2
摘要
Abstract Engineering the electronic band structures upon doping is crucial to improve the thermoelectric performance of materials. Understanding how dopants influence the electronic states near the Fermi level is thus a prerequisite to precisely tune band structures. Here, we demonstrate that the Sn-s states in SnTe contribute to the density of states at the top of the valence band. This is a consequence of the half-filled p-p σ-bond (metavalent bonding) and its resulting symmetry of the orbital phases at the valence band maximum (L point of the Brillouin zone). This insight provides a recipe for identifying superior dopants. The overlap between the dopant s- and the Te p-state is maximized, if the spatial overlap of both orbitals is maximized and their energetic difference is minimized. This simple design rule has enabled us to screen out Al as a very efficient dopant to enhance the local density of states for SnTe. In conjunction with doping Sb to tune the carrier concentration and alloying with AgBiTe 2 to promote band convergence, as well as introducing dislocations to impede phonon propagation, a record-high average ZT of 1.15 between 300 and 873 K and a large ZT of 0.36 at 300 K is achieved in Sn 0.8 Al 0.08 Sb 0.15 Te-4%AgBiTe 2 .
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