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dc.contributor.authorTuan, P. H.en_US
dc.contributor.authorLiang, H. C.en_US
dc.contributor.authorTung, J. C.en_US
dc.contributor.authorChiang, P. Y.en_US
dc.contributor.authorHuang, K. F.en_US
dc.contributor.authorChen, Y. F.en_US
dc.date.accessioned2019-04-03T06:44:37Z-
dc.date.available2019-04-03T06:44:37Z-
dc.date.issued2015-12-07en_US
dc.identifier.issn2470-0045en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevE.92.062906en_US
dc.identifier.urihttp://hdl.handle.net/11536/129338-
dc.description.abstractThe coupling interaction between the driving source and the RLC network is explored and characterized as the effective impedance. The mathematical form of the derived effective impedance is verified to be identical to the meromorphic function of the singular billiards with a truncated basis. By using the derived impedance function, the resonant modes of the RLC network can be divided into the open-circuit and short-circuit states to manifest the evolution of eigenvalues and eigenstates from closed quantum billiards to the singular billiards with a truncated basis in the strongly coupled limit. The substantial differences of the wave patterns between the uncoupled and strongly coupled eigenmodes in the two-dimensional wave systems can be clearly revealed with the RLC network. Finally, the short-circuit resonant states are exploited to confirm that the experimental Chladni nodal-line patterns in the vibrating plate are the resonant modes subject to the strong coupling between the oscillation system and the driving source.en_US
dc.language.isoen_USen_US
dc.titleManifesting the evolution of eigenstates from quantum billiards to singular billiards in the strongly coupled limit with a truncated basis by using RLC networksen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevE.92.062906en_US
dc.identifier.journalPHYSICAL REVIEW Een_US
dc.citation.volume92en_US
dc.citation.issue6en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000366099900013en_US
dc.citation.woscount1en_US
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