Conductivity of Two-dimensional Dirac Electrons Close to Merging in Organic Conductor α-STF2I3 at Ambient Pressure

Abstract

The electric conductivity of Dirac electrons in the organic conductor $\alpha$-STF$_2$I$_3$ (STF = bis(ethylenedithio)diselenadithiafulvalene), which has an isostructure of ET(=bis(ethylenedithio)tetrathiafulvalene), has been theoretically studied using a two-dimensional tight-binding model in the presence of both impurity and electron-phonon (e-p) scatterings.In contrast to ET, which has a Dirac cone with almost isotropic velocity, STF provides a large anisotropy owing to a Dirac point that is close to merging. As a result, $\sigma_{x}$ becomes much larger than $\sigma_{y}$, where $\sigma_y$ and $\sigma_x$ are diagonal conductivities parallel and perpendicular to a stacking axis of molecules, respectively. With increasing temperature ($T$), $\sigma_x$ takes a broad maximum because of e-p scattering and $\sigma_y$ remains almost constant. The ratio $\sigma_x/\sigma_y$ is analyzed in terms of the band structure. Such an exotic conductivity of STF is compared with that of an experiment showing a good correspondence. Finally, $\sigma_x/\sigma_y$ values of ET and BETS(= bis(ethylenedithio)tetraselenafulvalene) are shown to demonstrate the dissimilarity with STF.