Observation of disorder-induced boundary localization
arXiv:2402.10989 · doi:10.1073/pnas.2422154122
Abstract
Bloch wavefunctions in crystals experience localization within the bulk when disorder is introduced, a phenomenon commonly known as Anderson localization. This effect is considered universal, being applicable to all types of waves, quantum or classical. However, the interaction between disorder and topology -- a concept that has profoundly transformed many branches of physics -- necessitates revisiting the original Anderson localization picture. For instance, in the recently discovered topological Anderson insulator, the introduction of disorder induces topological boundary states that can resist localization due to protection from line-gap topology. While line-gap topology applies to both Hermitian and non-Hermitian systems, non-Hermitian systems uniquely exhibit point-gap topology, which has no Hermitian counterparts and leads to the non-Hermitian skin effect. Here, we experimentally demonstrate disorder-induced point-gap topology in a non-Hermitian acoustic crystal. This crystal, with non-Hermitian disorder in nearest-neighbor couplings, exhibits the non-Hermitian skin effect, where all eigenstates localize at a boundary. Interestingly, the boundary where localization occurs -- either the left or right -- depends on the strength of the disorder. As the disorder strength increases, the direction of boundary localization can be reversed. Additionally, we observe a ``bipolar" skin effect, where boundary localization occurs at both the left and right boundaries when disorder is introduced in next-nearest-neighbor couplings. These findings experimentally reveal a non-Hermitian mechanism of disorder-induced localization that goes beyond the conventional framework of Anderson localization.
7 pages, 4 figures
References in corpus (35)
- Topological Insulators
- Topological insulators and superconductors
- Edge states and topological invariants of non-Hermitian systems
- Anderson Transitions
- Topological phases of non-Hermitian systems
- Symmetry and Topology in Non-Hermitian Physics
- Topological Origin of Non-Hermitian Skin Effects
- Correspondence between winding numbers and skin modes in non-hermitian systems
- Observation of bulk boundary correspondence breakdown in topolectrical circuits
- Non-Hermitian Boundary Modes
- Observation of non-Hermitian bulk-boundary correspondence in quantum dynamics
- Efficient Light Funneling based on the non-Hermitian Skin Effect
- Topological Anderson Insulator
- Non-Hermitian Topological Invariants in Real Space
- Theory of the topological Anderson insulator
- Observation of the topological Anderson insulator in disordered atomic wires
- Photonic Topological Anderson Insulators
- Acoustic non-Hermitian skin effect from twisted winding topology
- Topological Non-Hermitian skin effect
- Numerical study of the topological Anderson insulator in HgTe/CdTe quantum wells
- Topological Criticality in the Chiral-Symmetric AIII Class at Strong Disorder
- Disorder-induced Floquet Topological Insulators
- Experimental Observation of Higher-Order Topological Anderson Insulators
- Topological Anderson Insulator in Three Dimensions
- Observation of non-Hermitian topological Anderson insulator in quantum dynamics
- Skin effect and winding number in disordered non-Hermitian systems
- Non-Hermitian Topological Anderson Insulators
- Topological Anderson insulators in two-dimensional non-Hermitian disordered systems
- Anderson localization of electromagnetic waves in three dimensions
- Photonic topological Anderson insulators
- Real space topological invariant and higher-order topological Anderson insulator in two-dimensional non-Hermitian systems
- Scale-free localization and PT symmetry breaking from local non-Hermiticity
- Bulk-Bulk Correspondence in Disordered Non-Hermitian Systems
- Disorder-driven Phase Transitions of Second-order Non-Hermitian Skin Effects
- Topological Anderson Insulators in Systems without Time-Reversal Symmetry
Cited by in corpus (6)
- Universal non-Hermitian transport in disordered systems
- Unifying Anderson transitions and topological amplification in non-Hermitian chains
- Non-Hermitian higher-order topological insulators enabled by altermagnet engineering
- Recent progress on disorder-induced topological phases
- Inter-species topological phases via a dynamical gauge field
- Arbitrary Control of Non-Hermitian Skin Modes via Disorder and An Electric Field