González-García Luis A, Caballero-Benítez Santiago F, Paredes Rosario
Instituto de Física, Universidad Nacional Autónoma de México, Apartado Postal 20-364, México, D. F. 01000, Mexico.
CONACYT-Instituto Nacional de Astrofísica, Óptica y Electrónica, Calle Luis Enrique Erro No. 1, Sta. María Tonantzintla, Pue, CP 72840, Mexico.
Sci Rep. 2019 Jul 30;9(1):11049. doi: 10.1038/s41598-019-47279-1.
We investigate the effects of disorder and lattice geometry against localisation phenomena in a weakly interacting ultracold bosonic gas confined in a 2D optical lattice. The behaviour of the quantum fluid is studied at the mean-field level performing computational experiments, as a function of disorder strength for lattices of sizes similar to current experiments. Quantification of localisation, away from the Bose glass phase, was obtained directly from the stationary density profiles through a robust statistical analysis of the condensate component, as a function of the disorder amplitude. Our results show a smooth transition, or crossover, to localisation induced by disorder in square and triangular lattices. In contrast, associated to its larger tunneling amplitude, honeycomb lattices show absence of localisation for the same range of disorder strengths and same lattice amplitude, while also exhibiting partial localisation for large disorder amplitudes. We also conclude that the coordination number z have a partial influence on how fast this smooth transition occurs as the system size increases. Signatures of disorder are also found in the ground state energy spectrum, where a continuous distribution emerges instead of a distribution of sharp peaks proper to the system in the absence of disorder.
我们研究了无序和晶格几何结构对限制在二维光学晶格中的弱相互作用超冷玻色气体中局域化现象的影响。在平均场水平上,通过进行计算实验,研究了量子流体的行为,该行为是与当前实验尺寸相似的晶格的无序强度的函数。通过对凝聚态分量进行稳健的统计分析,直接从稳态密度分布中获得了远离玻色玻璃相的局域化量化结果,该结果是无序幅度的函数。我们的结果表明,在正方形和三角形晶格中,由无序诱导的局域化存在平滑过渡或交叉。相比之下,由于其较大的隧穿幅度,对于相同范围的无序强度和相同的晶格幅度,蜂窝晶格没有出现局域化,而在大无序幅度下也表现出部分局域化。我们还得出结论,配位数z对随着系统尺寸增加这种平滑过渡发生的速度有部分影响。在基态能谱中也发现了无序的特征,在没有无序的情况下,系统的能谱本应是尖锐峰的分布,而此时出现了连续分布。