2023
DOI: 10.1103/physrevresearch.5.023020
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Hermitian and non-Hermitian Weyl physics in synthetic three-dimensional piezoelectric phononic beams

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Cited by 7 publications
(3 citation statements)
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“…This phenomenon is also observed in the study of flexural waves within a piezoelectric metabeam. [ 305 ] Although the existence of a Weyl point does not necessitate PT symmetry, it is achieved by appropriately tuning gain and loss parameters. Indeed, the exploration of elastic wave manipulation in non‐Hermitian systems that do not necessarily adhere to PT symmetry has proven to be more fruitful, [ 37,300–304 ] including intelligent non‐Hermitian MM systems.…”
Section: Intelligent Parity‐time Symmetric Mmsmentioning
confidence: 99%
See 1 more Smart Citation
“…This phenomenon is also observed in the study of flexural waves within a piezoelectric metabeam. [ 305 ] Although the existence of a Weyl point does not necessitate PT symmetry, it is achieved by appropriately tuning gain and loss parameters. Indeed, the exploration of elastic wave manipulation in non‐Hermitian systems that do not necessarily adhere to PT symmetry has proven to be more fruitful, [ 37,300–304 ] including intelligent non‐Hermitian MM systems.…”
Section: Intelligent Parity‐time Symmetric Mmsmentioning
confidence: 99%
“…Indeed, the exploration of elastic wave manipulation in non‐Hermitian systems that do not necessarily adhere to PT symmetry has proven to be more fruitful, [ 37,300–304 ] including intelligent non‐Hermitian MM systems. [ 305–309 ] This is attributed to the absence of the requirement for strict balance between gain and loss in such systems. Although there have been some recent studies on non‐Hermitian elastic MMs with or without PT symmetry, how to realize experimental implementation and even intelligent manipulation is still worthy of further research.…”
Section: Intelligent Parity‐time Symmetric Mmsmentioning
confidence: 99%
“…The first category involves the inclusion of non-Hermitian features in existing acoustic topological systems, which modifies the topological states in the presence of non-Hermiticity. For example, for an acoustic Weyl semimetal, the Weyl points will spread to Weyl exceptional rings in the presence of non-Hermiticity introduced by gain and loss [144,213]. Incorporating non-Hermiticity also modifies the bulk-boundary correspondence for topological insulators, leading to the so-called non-Hermitian skin effect (NHSE) which has been actively researched in the following areas of acoustics: (1) NHSE modifies the wave functions of TMs by adding directional responses, leading to chiral transportation [214] and directional amplification/decay of TMs [129,215]; (2) NHSE endows the topological edge modes with further spatial confinement, where directional transport owing to NHSEs results in wave accumulated at certain corners and hence forming a higher-order topological insulators supporting corner states [153,216,217] (figures 12(a) and (b)); (3) NHSE can modify the wave functions of TMs by delocalization, which leads to a topological state spreading in the bulk and hence is called the Extended State in a Localized Continuum [218]; (4) More generally, there is a competition between NHSEs and TMs, and thus NHSE can be used to arbitrarily morph the wavefunctions [154].…”
Section: Non-hermitian Acoustics In Topological Systemsmentioning
confidence: 99%