The platform will undergo maintenance on Sep 14 at about 9:30 AM EST and will be unavailable for approximately 1 hour.
2021
DOI: 10.1007/s11433-021-1802-4
|View full text |Cite
|
Sign up to set email alerts
|

Exact mobility edges and topological phase transition in two-dimensional non-Hermitian quasicrystals

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
5

Citation Types

0
6
0

Year Published

2021
2021
2023
2023

Publication Types

Select...
7
2

Relationship

0
9

Authors

Journals

citations
Cited by 23 publications
(7 citation statements)
references
References 84 publications
0
6
0
Order By: Relevance
“…Novel transport phases and topological phases are found when hoppings are long ranged [38][39][40] or quasiperiodic as well [41]. Besides these, twodimensional (2D) quasiperiodic systems provide richer phenomena of localization [42,43], topology [44], flat band [45], and many-body effects [23,46].…”
Section: Introductionmentioning
confidence: 99%
“…Novel transport phases and topological phases are found when hoppings are long ranged [38][39][40] or quasiperiodic as well [41]. Besides these, twodimensional (2D) quasiperiodic systems provide richer phenomena of localization [42,43], topology [44], flat band [45], and many-body effects [23,46].…”
Section: Introductionmentioning
confidence: 99%
“…Novel transport phases and topological phases are found when hoppings are long ranged [38][39][40] or quasiperiodic as well [41]. Besides these, two-dimensional (2D) quasiperiodic systems provide richer phenomena of localization [42,43], topology [44], flat band [45], and many-body effects [23,46].…”
Section: Introductionmentioning
confidence: 99%
“…In realistic experiments, the loss cannot be completely avoided due to the coupling of systems to the environment or measurement [11]; for cold atoms, few-body losses play inevitable roles in the preparation of degenerate quantum gases [2] and in the simulation of quantum many-body physics [3]. On the other hand, the non-Hermitian physics attracts increasing attention of almost all branches of physics in recent years [12], where abundant exotic phenomena, such as the spontaneous breaking of the parity-time (PT ) symmetry [13][14][15][16][17][18], the breakdown of the conventional bulk-boundary correspondence [19][20][21][22][23][24][25][26][27][28][29], the exceptional topology [30], and the interplay with Anderson localization [31][32][33][34][35][36][37], have been widely exploited both in theory and experiment. As for cold atoms, the experimental techniques are mature to engineer state-dependent atom losses [17,18] and the effective nonreciprocal hoppings [38] of non-Hermitian systems, which are fundamental operations for the construction of a non-Hermitian model.…”
Section: Introductionmentioning
confidence: 99%