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arXiv 2006.01182cond-mat.str-elcond-mat.othercond-mat.quant-gasnlin.CGquant-ph
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无开边界的多体拓扑与皮肤态

Many-Body Topological and Skin States without Open Boundaries

Ching Hua Lee

摘要:

鲁棒边界态一直是最近研究的焦点,无论是作为拓扑保护态还是作为非厄米皮肤态。在这项工作中,我们表明,多体效应也可以诱导这些强大的国家在实际的物理边界的地方类似物。粒子统计或适当设计的相互作用(即在超冷原子晶格中)可以限制可访问的多体希尔伯特空间,并在空间周期性高维配置空间中引入有效边界。我们证明了拓扑手征模式的出现在一个两个费米子跳跃模型没有开放的边界,费米子对限制和适当选择的通量不对称传播。跨不同粒子种类的异质非互易跳跃也可以导致平移不变设置中的鲁棒粒子聚集,这让人想起开放边界处的皮肤模式累积。但与固定的开放边界不同,有效边界对应于不可穿透粒子的位置,并且是动态的,从而产生了根本不同的多体与单体时间演化行为。由于非互易积累是不可知的限制希尔伯特空间的维数,我们的多体皮肤状态直接推广的热力学极限。然而,多体拓扑态具有非平凡的维数依赖性,对多体拓扑态的详细研究将促进对高维拓扑不变量的进一步研究。

英文摘要:

Robust boundary states have been the focus of much recent research, both as topologically protected states and as non-Hermitian skin states. In this work, we show that many-body effects can also induce analogs of these robust states in place of actual physical boundaries. Particle statistics or suitably engineered interactions i.e. in ultracold atomic lattices can restrict the accessible many-body Hilbert space, and introduce effective boundaries in a spatially periodic higher-dimensional configuration space. We demonstrate the emergence of topological chiral modes in a two-fermion hopping model without open boundaries, with fermion pairs confined and asymmetrically propagated by suitably chosen fluxes. Heterogeneous non-reciprocal hoppings across different particle species can also result in robust particle clumping in a translation invariant setting, reminiscent of skin mode accumulation at an open boundary. But unlike fixed open boundaries, effective boundaries correspond to the locations of impenetrable particles and are dynamic, giving rise to fundamentally different many-body vs. single-body time evolution behavior. Since non-reciprocal accumulation is agnostic to the dimensionality of restricted Hilbert spaces, our many-body skin states generalize directly in the thermodynamic limit. The many-body topological states, however, are nontrivially dimension-dependent, and their detailed exploration will stimulate further studies in higher dimensional topological invariants.

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