2015
DOI: 10.1103/physreva.91.033825
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Parity-time symmetry from stacking purely dielectric and magnetic slabs

Abstract: We show that Parity-time symmetry in matching electric permittivity to magnetic permeability can be established by considering an effective Parity operator involving both mirror symmetry and coupling between electric and magnetic fields. This approach extends the discussion of Parity-time symmetry to the situation with more than one material potential. We show that the band structure of a one-dimensional photonic crystal with alternating purely dielectric and purely magnetic slabs can undergo a phase transitio… Show more

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Cited by 53 publications
(35 citation statements)
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“…[36] and they can be chosen by the way of excitation, e.g., the symmetry of incident waves hereby. Interestingly, our system exhibits the cross-matched P T symmetry, i.e., ε(x) = μ * (−x) [37].…”
Section: Discussionmentioning
confidence: 97%
“…[36] and they can be chosen by the way of excitation, e.g., the symmetry of incident waves hereby. Interestingly, our system exhibits the cross-matched P T symmetry, i.e., ε(x) = μ * (−x) [37].…”
Section: Discussionmentioning
confidence: 97%
“…Interestingly, Li et al explored the possibility of cross-matching ε(z) to μ * (−z), namely, ε(z) = μ * (−z), to establish PT symmetry [87]. More specifically, they investigated a 1D photonic crystal (PhC) consisting of alternating purely dielectric slabs with ε 1 = 2.25 + iγ, μ 1 = 1 and purely magnetic slabs with μ 2 = 2.25 − iγ, ε 2 = 1 ( Figure 6A).…”
Section: Unidirectional Reflectionless Propagation In Pt-symmetric Symentioning
confidence: 99%
“…is the eigenvalue of (6), not the Bloch wavenumber k z ; however it is natural to investigate the characteristics of k z since it allows for a straightforward assessment of the gain and loss balance [71]. Bloch eigenmodes that satisfy (3) and (6) are derived from the eigenvalue problem,…”
Section: A State Vector Evolution and Transfer Matrixmentioning
confidence: 99%