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Seebeck Effect of Dirac Electrons in Organic Conductors under Hydrostatic Pressure Using a Tight-Binding Model Derived from First Principles
Journal of the Physical Society of Japan ( IF 1.7 ) Pub Date : 2024-04-08 , DOI: 10.7566/jpsj.93.054704
Yoshikazu Suzumura, Takao Tsumuraya, Masao Ogata

The Seebeck coefficient is examined for two-dimensional Dirac electrons in the three-quarter filled organic conductor α-(BEDT-TTF)2I3 [BEDT-TTF denotes bis(ethylenedithio)tetrathiafulvalene] under hydrostatic pressure, where the Seebeck coefficient S is proportional to the ratio of the thermoelectric conductivity L12 to the electrical conductivity L11, i.e., S = L12/TL11 with T being the temperature. We present an improved tight-binding model in two dimensions with transfer energies determined from first-principles density functional theory calculations with an experimentally determined crystal structure. The T dependence of the Seebeck coefficient is calculated by adding impurity and electron–phonon scatterings. Noting a zero-gap state due to the Dirac cone, which results in a competition from contributions between the conduction and valence bands, we show positive Sx and Sy at finite temperatures and analyze them in terms of spectral conductivity. The relevance of the calculated Sx (perpendicular to the molecular stacking axis) to the experiment is discussed.

中文翻译:

使用源自第一原理的紧束缚模型研究静水压力下有机导体中狄拉克电子的塞贝克效应

检查静水压力下四分之三填充有机导体α -(BEDT-TTF) 2 I 3 [BEDT-TTF 表示双(乙撑二硫)四硫富瓦烯]中二维狄拉克电子的塞贝克系数,其中塞贝克系数S为与热电导率L 12与电导率L 11的比值成正比,即SL 12 / TL 11其中T为温度。我们提出了一种改进的二维紧束缚模型,其转移能是根据第一原理密度泛函理论计算和实验确定的晶体结构确定的。塞贝克系数的T依赖性是通过添加杂质和电子声子散射来计算的。注意到狄拉克锥导致的零能隙状态,导致导带和价带之间的贡献竞争,我们在有限温度下显示正的S xS y,并根据光谱电导率对它们进行分析。讨论了计算出的S x(垂直于分子堆积轴)与实验的相关性。
更新日期:2024-04-08
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