2020
DOI: 10.1103/physrevb.102.161101
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Untying links through anti-parity-time-symmetric coupling

Abstract: We reveal how the vector field links are untied under the influence of anti-parity-time-symmetric couplings in a dissipative sublattice-symmetric topological photonic crystal lattice. The topology of the quasi-one-dimensional two-band system is encoded in the geometric topology of the vector fields associated with the Bloch Hamiltonian. The linked vector fields reflect the topology of the nontrivial phase. The topological phase transition occurs concomitantly with the untying of the vector field link at the ex… Show more

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Cited by 36 publications
(18 citation statements)
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“…In this section, we study the properties of an anti-PT -symmetric non-Hermitian scattering center, which is a four-site scattering center with imaginary coupling. The imaginary coupling can be realized through dissipation in the non-Hermitian systems [56]. The schematic of the anti-PT -symmetric non-Hermitian system is shown in Fig.…”
Section: Nonunitary Scatteringmentioning
confidence: 99%
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“…In this section, we study the properties of an anti-PT -symmetric non-Hermitian scattering center, which is a four-site scattering center with imaginary coupling. The imaginary coupling can be realized through dissipation in the non-Hermitian systems [56]. The schematic of the anti-PT -symmetric non-Hermitian system is shown in Fig.…”
Section: Nonunitary Scatteringmentioning
confidence: 99%
“…Notably, each dot in the schematics represents a primary resonator and each line between the two neighbor primary resonators represents the effective coupling induced by the linking resonator after adiabatically eliminating the linking resonator. The effective coupling induced by the off-resonance passive linking resonator without dissipation/gain is real and Hermitian [67]; in contrast, the effective coupling induced by the on-resonance dissipative/active linking resonator with dissipative/gain is imaginary and non-Hermitian [56,60]. In the two situations, the effective coupling strength is approximately equal to the product of the two couplings between the linking resonator and its two adjacent primary resonators divided by the off-resonant frequency or the dissipation/gain rate of the linking resonator.…”
Section: Experimental Realizationmentioning
confidence: 99%
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“…The resonator detuning ∆ j is real. The coupling iγ j is non-Hermitian and can be realized through the gain [64,109]. The scattering center H c is pseudo-Hermitian for the unitary matrix q = I 3 ⊗ σ z .…”
mentioning
confidence: 99%