论文标题

特殊点在非铁人Lieb晶格中成为星体:进化和拓扑保护

Exceptional points make an astroid in non-Hermitian Lieb lattice: evolution and topological protection

论文作者

Xiao, Yi-Xin, Ding, Kun, Zhang, Ruo-Yang, Hang, Zhi Hong, Chan, C. T.

论文摘要

在非高核心时,发现了一个由四个尖端组成的特殊点(EPS)(EPS)(EPS)(EPS)(EPS),包括四个尖头,是从Brillouin区(BZ)的三重脱位点(BZ)产生的,该晶格是在非热质性的情况下带来的,它具有最近的neighbor Hoppings。 EP回路的发生是由于判别物的真实性,这是由非弱者手性对称性保证的。四个尖端的EPS涉及三个本征态的合并,这是非热性手性对称性和镜像对称性的综合结果。 EP循环正是无限非电性极限的星体。 EP循环从$ m $点扩展,非热度增加,并以关键的非热度分为两个EP循环。非热性的进一步提高与BZ中的$ x $和$ y $点的两个EP循环,最后提高到两个EPS,并伴随着Diraclike圆锥体的出现。这两个EP在较大的非热性上消失。 EP环消失,当引入最新的跳动以打破非富甲性手性对称性时,发现几个离散的EP可以生存。一种称为判别数的拓扑不变式来表征其对扰动的鲁棒性。发现EPS和EP环上的EPS都显示出各向异性渐近行为。最后,讨论了使用耦合波导阵列对LIEB晶格的实验实现。

An astroid-shaped loop of exceptional points (EPs), comprising four cusps, is found to spawn from the triple degeneracy point in the Brillouin zone (BZ) of a Lieb lattice with nearest-neighbor hoppings when non-Hermiticity is introduced. The occurrence of the EP loop is due to the realness of the discriminant which is guaranteed by the non-Hermitian chiral symmetry. The EPs at the four cusps involve the coalescence of three eigenstates, which is the combined result of the non-Hermitian chiral symmetry and mirror-T symmetry. The EP loop is exactly an astroid in the limit of an infinitesimal non-Hermiticity. The EP loop expands from the $M$ point with increasing non-Hermiticity and splits into two EP loops at a critical non-Hermiticity. The further increase of non-Hermiticity contracts the two EP loops towards and finally to two EPs at the $X$ and $Y$ points in the BZ, accompanied by the emergence of Dirac-like cones. The two EPs vanish at a larger non-Hermiticity. The EP loop disappears and several discrete EPs are found to survive when next-nearest hoppings are introduced to break the non-Hermitian chiral symmetry. A topological invariant called the discriminant number is used to characterize their robustness against perturbations. Both discrete EPs and those on the EP loop(s) are found to show anisotropic asymptotic behaviors. Finally, the experimental realization of the Lieb lattice using a coupled waveguide array is discussed.

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