First-principles study of the effective Hamiltonian for Dirac fermions with spin-orbit coupling in two-dimensional molecular conductor $\alpha$-(BETS)$_2$I$_3$
First-principles study of the effective Hamiltonian for Dirac fermions with spin-orbit coupling in two-dimensional molecular conductor $\alpha$-(BETS)$_2$I$_3$
复制标题
二维分子导体$alpha$-(BETS)$_2$I$_3$中自旋轨道耦合狄拉克费米子有效哈密顿量的第一性原理研究
DOI:
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发表时间:
2020
期刊:
影响因子:
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通讯作者:
Y. Suzumura
中科院分区:
文献类型:
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作者:
T. Tsumuraya;Y. Suzumura
We study the electronic states associated with Dirac electrons in quasi-two-dimensional molecular conductor $\alpha$-(BETS)$_2$I$_3$ [= $\alpha$-(BEDT-TSeF)$_2$I$_3$] using first-principles density-functional theory (DFT) calculations. Using a low-temperature structure of 30K, we provide a tight-binding (TB) model with intermolecular transfer energies evaluated from maximally-localized Wannier functions (MLWFs). The TB model for the molecular solid is complicated; the number of relevant transfer integral is relatively large due to the delocalized character of Se $p$ orbitals. We demonstrate exotic behaviors of both cases of a zero-gap state (ZGS) with massless Dirac dispersion and an insulating state with an indirect band gap of about 2 meV. The former model parameters are extracted from a scalar-relativistic DFT calculation in the absence of spin-orbit coupling (SOC), and those of the latter model are obtained from the full-relativistic calculation in the presence of SOC. The energy spectrum close to the Dirac point is analyzed by comparing it with some eigenvalues at the time-reversal invariant momentum (TRIM). A precise effective Hamiltonian is developed using MLWFs generated from Bloch functions obtained in self-consistent full-relativistic DFT calculations. We also determined site-potentials that give the spectrum corresponding to the DFT bands by a reasonable fitting.