dorsal/arxiv
View SchemaSpectral Distribution of one-dimensional Photonic Quasicrystals: The Role of Irrational Numbers
| Authors | Hui Quan, Wei Si, Kai Jiang |
|---|---|
| Categories | |
| ArXiv ID | 2601.06482vv1 |
| URL | https://arxiv.org/abs/2601.06482 |
| License | http://creativecommons.org/licenses/by/4.0/ |
Abstract
In this paper, we construct a one-dimensional photonic quasicrystal by combining two incommensurate spatial harmonics, where the ratio of their periods is the irrational number \beta. We evaluate the photonic quasicrystal accurately by a generalized spectral method that embeds the quasiperiodic structure into a higher-dimensional periodic system. We study the spectral distribution of one-dimensional photonic quasicrystals and find some interesting phenomena. As the computational resolution N increases, there are more eigenvalues within finite frequency bandwidths, and the maximum localization always occurs at spectral gap edges for states near index N + 1. By varying \beta within the range of (0,1), we present a butterfly-shaped spectral structure with abundant band gaps. We find that the spectral structure factor Q (defined as I_{mg}/N, where I_{mg} is the maximum gap index) exhibits different linear patterns as \beta changes: Q = 1 - \beta when \beta < \beta c, while Q = \beta when \beta > \beta c, where \beta c \approx 0.424 is the transition point. This linear relationship holds robustly in the strong quasiperiodic regime (\beta away from 0 or 1) and is independent of the specific type of irrational number used. The relationship disappears (weak quasiperiodic regime) near \beta = 0 or \beta = 1. It demonstrates that the intrinsic spectral properties of one-dimensional photonic quasicrystals are fundamentally governed by the magnitude of the irrational parameter \beta.
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"abstract": "In this paper, we construct a one-dimensional photonic quasicrystal by combining two incommensurate spatial harmonics, where the ratio of their periods is the irrational number \\beta. We evaluate the photonic quasicrystal accurately by a generalized spectral method that embeds the quasiperiodic structure into a higher-dimensional periodic system. We study the spectral distribution of one-dimensional photonic quasicrystals and find some interesting phenomena. As the computational resolution N increases, there are more eigenvalues within finite frequency bandwidths, and the maximum localization always occurs at spectral gap edges for states near index N + 1. By varying \\beta within the range of (0,1), we present a butterfly-shaped spectral structure with abundant band gaps. We find that the spectral structure factor Q (defined as I_{mg}/N, where I_{mg} is the maximum gap index) exhibits different linear patterns as \\beta changes: Q = 1 - \\beta when \\beta \u003c \\beta c, while Q = \\beta when \\beta \u003e \\beta c, where \\beta c \\approx 0.424 is the transition point. This linear relationship holds robustly in the strong quasiperiodic regime (\\beta away from 0 or 1) and is independent of the specific type of irrational number used. The relationship disappears (weak quasiperiodic regime) near \\beta = 0 or \\beta = 1. It demonstrates that the intrinsic spectral properties of one-dimensional photonic quasicrystals are fundamentally governed by the magnitude of the irrational parameter \\beta.",
"arxiv_id": "2601.06482",
"authors": [
"Hui Quan",
"Wei Si",
"Kai Jiang"
],
"categories": [
"physics.optics"
],
"license": "http://creativecommons.org/licenses/by/4.0/",
"title": "Spectral Distribution of one-dimensional Photonic Quasicrystals: The Role of Irrational Numbers",
"url": "https://arxiv.org/abs/2601.06482",
"version": "v1"
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