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Slave-boson mean-field theory of the Mott transition in the two-band Hubbard model

机译:两频带Hubbard模型中Mott跃迁的从玻色子平均场理论

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We apply the slave-boson approach of Kotliar and Ruckenstein to the two-band Hubbard model with an Ising like Hund's rule coupling and bands of different widths. On the mean-field level of this approach we investigate the Mott transition and observe both separate and joint transitions of the two bands depending on the choice of the inter- and intra-orbital Coulomb interaction parameters. The mean-field calculations allow for a simple physical interpretation and can confirm several aspects of previous work. Beside the case of two individually half-filled bands we also examine what happens if the original metallic bands possess fractional filling either due to finite doping or due to a crystal field which relatively shifts the atomic energy levels of the two orbitals. For appropriate values of the interaction and of the crystal field we can observe a band insulating state and a ferromagnetic metal.
机译:我们将Kotliar和Ruckenstein的奴隶玻色方法应用于具有Ising像Hund的规则耦合和不同宽度的带的两带Hubbard模型。在这种方法的平均场水平上,我们根据轨道间和轨道内库仑相互作用参数的选择,研究了莫特跃迁并观察了两个频带的分离跃迁和联合跃迁。平均场计算可以进行简单的物理解释,并且可以确认以前的工作的几个方面。除了两个单独的半填充带以外,我们还研究了如果原始金属带由于有限的掺杂或由于相对于两个轨道的原子能级相对移动的晶体场而具有部分填充的情况,会发生什么情况。对于相互作用和晶体场的适当值,我们可以观察到能带绝缘状态和铁磁金属。

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