In a PT-symmetric 1D moiré lattice, the parity of the commensurate ratio denominator determines which band pair first breaks PT symmetry, controlling whether the lowest flat band broadens monotonically (even denominators) or nonmonotonically (odd denominators).
Three-dimensional Coupled PT-symmetric Electronic Resonators
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abstract
In this article, the non-Hermitian characteristics of three-dimensional PT-symmetric coupled electronic resonators are theoretically analyzed. First, the concept of non-Hermitian PT symmetry is illustrated in the context of electronics using a pair of coupled electronic resonators. Two typical configurations of parallel-coupled PT-symmetric electronic trimers are then analyzed. The results indicate that, for the planar configuration, the system can exhibit two phase transitions as the coupling coefficient or gain-loss parameter changes, different from the linear configuration. By comparing system equations based on coupled-mode theory and circuit theory, it is shown that high dimensionality alone is not a sufficient condition for the existence of a higher-order exceptional point; an approximation condition is also required. A modified exceptional point is proposed, and the approximation conditions for the mean deviation $D$ for the real part of the three eigenfrequencies, satisfying $D \leq 1\%$ and $D \leq 0.1\%$, are discussed, respectively. The theoretical results presented in this paper not only reveal the unique non-Hermitian characteristics of high-dimensional PT-symmetric electronic systems but also offer theoretical support for wireless power transmission and wireless sensing technologies.
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cond-mat.quant-gas 1years
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Fate of moir\'e flat bands for a weakly repulsive Bose-Einstein condensate in one-dimensional $\mathcal{PT}$-symmetric bichromatic optical lattices
In a PT-symmetric 1D moiré lattice, the parity of the commensurate ratio denominator determines which band pair first breaks PT symmetry, controlling whether the lowest flat band broadens monotonically (even denominators) or nonmonotonically (odd denominators).