In a disordered dissipative quantum link chain, a reciprocal cyclic boundary condition preserves the reduced steady-state matter occupations fixed by the accumulated dissipative disorder field while altering the Liouvillian spectrum to accelerate relaxation relative to open boundaries.
Title resolution pending
4 Pith papers cite this work. Polarity classification is still indexing.
4
Pith papers citing it
citation-role summary
background 1
method 1
citation-polarity summary
years
2026 4verdicts
UNVERDICTED 4representative citing papers
The localization length of the non-Hermitian skin effect is encoded in the quantum metric of right eigenstates, exhibiting power-law divergences at gapless points and discontinuities at cusps of the generalized Brillouin zone.
The non-Hermitian winding number of the reflection matrix links to the bulk Floquet invariant through boundary resonances, and the momentum-integrated Goos-Hänchen shift quantitatively measures the gap's topological invariant.
Non-Hermitian Floquet systems host gapless symmetry-protected topological phases with unified winding numbers and robust edge modes surviving at criticality.
citing papers explorer
-
Boundary-Controlled Liouvillian Relaxation with Exact Steady States Fixed by Dissipative Disorder
In a disordered dissipative quantum link chain, a reciprocal cyclic boundary condition preserves the reduced steady-state matter occupations fixed by the accumulated dissipative disorder field while altering the Liouvillian spectrum to accelerate relaxation relative to open boundaries.
-
Quantum geometry of the non-Hermitian skin effect
The localization length of the non-Hermitian skin effect is encoded in the quantum metric of right eigenstates, exhibiting power-law divergences at gapless points and discontinuities at cusps of the generalized Brillouin zone.
-
Probing Floquet topological phases via non-Hermitian skin effect of reflected waves
The non-Hermitian winding number of the reflection matrix links to the bulk Floquet invariant through boundary resonances, and the momentum-integrated Goos-Hänchen shift quantitatively measures the gap's topological invariant.
-
Topology and edge modes surviving criticality in non-Hermitian Floquet systems
Non-Hermitian Floquet systems host gapless symmetry-protected topological phases with unified winding numbers and robust edge modes surviving at criticality.