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Effect of disorder on the interacting Fermi gases in a one-dimensional optical lattice

机译:一维光学晶格中无序对相互作用费米气体的影响

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摘要

Interacting two-component Fermi gases loaded in a one-dimensional (1D) lattice and subjected to a harmonic trapping potential exhibit interesting compound phases in which fluid regions coexist with local Mott-insulator and/or band-insulator regions. Motivated by experiments on cold atoms inside disordered optical lattices, we present a theoretical study of the effects of a correlated random potential on these ground-state phases. We employ a lattice version of density-functional theory within the local-density approximation to determine the density distribution of fermions in these phases. The exchange-correlation potential is obtained from the Lieb-Wu exact solution of Fermi-Hubbard model. On-site disorder (with and without Gaussian correlations) and harmonic trap are treated as external potentials. We find that disorder has two main effects: (i) it destroys the local insulating regions if it is sufficiently strong compared with the on-site atom-atom repulsion, and (ii) it induces an anomaly in the inverse compressibility at low density from quenching of percolation. For sufficiently large disorder correlation length the enhancement in the inverse compressibility diminishes. © 2008 World Scientific Publishing Company.
机译:加载在一维(1D)晶格中并受到谐波俘获电势的相互作用的两组分费米气体表现出有趣的复合相,其中流体区域与局部Mott绝缘体和/或带绝缘体区域共存。通过对无序光学晶格内的冷原子进行实验的激励,我们提出了对相关随机势对这些基态相的影响的理论研究。我们在局部密度近似中采用密度泛函理论的晶格形式,以确定这些相中费米子的密度分布。交换相关势是从费米-哈伯德模型的Lieb-Wu精确解中获得的。现场无序(具有和没有高斯相关性)和谐波陷阱被视为外部电位。我们发现无序具有两个主要作用:(i)如果与现场原子-原子排斥相比足够强,它会破坏局部绝缘区域;(ii)在低密度下,它会引起反向压缩性异常渗流淬灭。对于足够大的无序相关长度,逆压缩性的增强减小。 ©2008世界科学出版公司。

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