arXiv:2604.24883cond-mat.quant-gascond-mat.supr-con2026-04

用神经网络发现二维自旋不平衡费米气体中新型配对态

Uncovering Exotic Paired States in the 2D Spin-Imbalanced Fermi Gas with Neural Wave Functions

论文配图:Uncovering Exotic Paired States in the 2D Spin-Imbalanced Fermi Gas with Neural Wave Functions
图 1 · 摘自论文原文
  • 用神经波函数方法模拟强关联自旋不平衡费米气体
  • 发现强相互作用下少数自旋粒子动量密度趋近于零
  • 观测到库珀对晶体与相分离共存的奇异物态,适合超冷原子研究者

我们采用基于AGPs FermiNet变分蒙特卡洛方法,研究短程吸引相互作用下二维自旋不平衡费米气体在零温下的相图。在弱相互作用的BCS极限下观察到Fulde-Ferrell-Larkin-Ovchinnikov相,在强相互作用的BEC极限下出现极化超流体。当相互作用较强时,少数自旋的动量空间密度在多数自旋占据的动量区域几乎降为零;当相互作用极强时,系统发生相分离,形成由玻色子对构成的区域和剩余多数自旋粒子占据的未配对区域。此外,在中等相互作用强度下,系统出现平移对称性破缺,形成库珀对晶体镶嵌在未配对多数自旋费米液体中的奇异晶格结构。本文还解释了强束缚情况下动量空间空洞的起源,并讨论该方法对未来研究的启示。

原文摘要 · Abstract (English)

We study the zero-temperature phase diagram of the 2D spin-imbalanced Fermi gas with short-ranged attractive interactions using the recently developed neural network variational Monte Carlo method with the AGPs FermiNet Ansatz. The Fulde-Ferrell-Larkin-Ovchinnikov phase is observed in the weakly interacting BCS limit and a polarised superfluid is seen in the strongly interacting BEC limit. When the interactions are strong, the minority-spin momentum density is reduced almost to zero in the momentum-space region occupied by the unpaired majority-spin electrons. When the interactions are very strong, phase separation occurs, with regions containing bosonic pairs and unpaired regions occupied by the remaining majority-spin particles. In addition, we observe translational symmetry breaking at intermediate interaction strengths, where the system forms an exotic crystal of Cooper pairs in a Fermi fluid of unpaired majority-spin particles. We provide a possible explanation for the formation of the crystalline phase, explain the origins of the k-space momentum-density hole when the pairs are tightly bound, and discuss how our approach opens new directions for future work.

量子模拟超导神经网络费米气体

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