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PreprintCC BY-NC-ND 4.0arXiv

Band-Edge Homogenization and the Sound-Soft Limit of Finite Bubbly Crystals

Abstract

We establish a quantitative sound-soft scattering limit for a finite bubbly crystal near the upper edge of the first Bloch band of the corresponding infinite crystal. The inclusions form a dense periodic array of period ε in a bounded Lipschitz domain, and their density contrast is δ=ε2, with fixed positive wave speeds. Under coordinate-reflection symmetry, we prove that the normalized capacitance symbol has a unique nondegenerate maximum on the Brillouin torus. Its Hessian defines a positive Dirichlet elliptic operator governing the limiting spectral detunings. A mean-constrained variational formulation allows us to compare the actual finite-array capacitance matrix with the truncated infinite-lattice operator and to prove exponential localization of their difference near the sample boundary. We obtain an O(ε) norm-resolvent approximation and connect it to the full acoustic scattering problem, retaining the second-order Bloch correction required by the frequency scaling. For rescaled detunings outside the effective Dirichlet spectrum, the exterior L2 and far-field discrepancies are O(ε), while the interior L2 field is O(ε1/2). Numerical experiments illustrate the far-field convergence and the effective spectral modes. Explicit one-dimensional calculations describe finer Fabry--Pérot transmission windows and show that a fixed frequency strictly inside the first band need not have a unique scattering limit.

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BibTeX
@misc{ammari2026bandedge,
  title = {{Band-Edge Homogenization and the Sound-Soft Limit of Finite Bubbly Crystals}},
  author = {Habib Ammari and Yuxin Du and Xin Fu and Wenjia Jing and Moritz Melcher},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.27494},
  eprint = {2609.27494},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.27494},
  note = {CC BY-NC-ND 4.0},
}
RIS
TY  - UNPB
TI  - Band-Edge Homogenization and the Sound-Soft Limit of Finite Bubbly Crystals
AU  - Habib Ammari
AU  - Yuxin Du
AU  - Xin Fu
AU  - Wenjia Jing
AU  - Moritz Melcher
PY  - 2026
DA  - 2026/09/23
PB  - arXiv
DO  - 10.48550/arxiv.2609.27494
UR  - https://arxiv.org/abs/2609.27494
AB  - We establish a quantitative sound-soft scattering limit for a finite bubbly crystal near the upper edge of the first Bloch band of the corresponding infinite crystal. The inclusions form a dense periodic array of period ε in a bounded Lipschitz domain, and their density contrast is δ=ε^2, with fixed positive wave speeds. Under coordinate-reflection symmetry, we prove that the normalized capacitance symbol has a unique nondegenerate maximum on the Brillouin torus. Its Hessian defines a positive Dirichlet elliptic operator governing the limiting spectral detunings. A mean-constrained variational formulation allows us to compare the actual finite-array capacitance matrix with the truncated infinite-lattice operator and to prove exponential localization of their difference near the sample boundary. We obtain an O(ε) norm-resolvent approximation and connect it to the full acoustic scattering problem, retaining the second-order Bloch correction required by the frequency scaling. For rescaled detunings outside the effective Dirichlet spectrum, the exterior L^2 and far-field discrepancies are O(ε), while the interior L^2 field is O(ε^1/2). Numerical experiments illustrate the far-field convergence and the effective spectral modes. Explicit one-dimensional calculations describe finer Fabry--Pérot transmission windows and show that a fixed frequency strictly inside the first band need not have a unique scattering limit.
ER  -