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Many-body-localization transition: strong multifractality spectrum for matrix elements of local operators

机译:多体定位过渡:局部算子矩阵元素的强多重分形谱

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For short-ranged disordered quantum models in one dimension, the many-body-localization is analyzed via the adaptation to the many-body context (Serbyn et al 2015 Phys. Rev. X 5 041047) of the Thouless point of view on the Anderson transition: the question is whether a local interaction between two long chains is able to reshuffle completely the eigenstates (delocalized phase with a volume-law entanglement) or whether the hybridization between tensor states remains limited (many-body-localized phase with an area-law entanglement). The central object is thus the level of hybridization induced by the matrix elements of local operators, as compared with the difference of diagonal energies. The multifractal analysis of these matrix elements of local operators is used to analyze the corresponding statistics of resonances. Our main conclusion is that the critical point is characterized by the strong-multifractality spectrum f(0 <= alpha <= 2) = alpha/2, well known in the context of Anderson localization in spaces of effective infinite dimensionality, where the size of the Hilbert space grows exponentially with the volume. Finally, the possibility of a delocalized non-ergodic phase near criticality is discussed.
机译:对于在一维中的短距离无序量子模型,通过适应安德森一世观点的多体环境(Serbyn等人,2015 Phys。Rev. X 5 041047)来分析多体定位。过渡:问题是两个长链之间的局部相互作用是否能够完全改组本征态(具有体积律纠缠的离域相),或者张量状态之间的杂交是否仍然受到限制(具有区域面积的多体局部相?法律纠缠)。因此,中心对象是与对角能量的差相比,由本地算子的矩阵元素引起的杂交水平。对局部算子的这些矩阵元素的多重分形分析用于分析共振的相应统计量。我们的主要结论是,临界点的特征在于强多重分形谱f(0 <= alpha <= 2)= alpha / 2,这在有效无限维空间中安德森局部化的背景下众所周知,其中希尔伯特空间随体积呈指数增长。最后,讨论了在临界附近发生离域非遍历阶段的可能性。

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