FFLO Excitonic State in the Three-Chain Hubbard Model for TaNiSe
arXiv:1602.03248 · doi:10.7566/JPSJ.85.053703
Abstract
The three-chain Hubbard model for TaNiSe known as a candidate material for the excitonic insulator is investigated over the wide range of energy gap between the two-fold degenerate conduction bands and the nondegenerate valence band including both semiconducting () and semimetallic () cases. In the semimetallic case, the difference of the band degeneracy inevitably causes the imbalance of each Fermi wavenumber, resulting in a remarkable excitonic state characterized by the condensation of excitons with finite center-of-mass momentum , the so-called Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) excitonic state. With decreasing corresponding to increasing pressure, the obtained excitonic phase diagram shows a crossover from BEC ($D\simg 0$) to BCS ($D\siml 0$) regime, and then shows a distinct phase transition at a certain critical value from the uniform () to the FFLO () excitonic state, as expected to be observed in TaNiSe under high pressure.
5 pages, 4 figures, J. Phys. Soc. Jpn, in press
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