Skip to content
DraconiticResearch
Search Sources API
203,203 studies31 sourcesUpdated 26 min ago
PreprintarXiv licencearXiv

Interface-Shifted Minnaert Resonances

Abstract

We develop a unified asymptotic theory for Minnaert resonances generated by a small bubble Dε placed near an interface Γ of material discontinuity in an acoustic background. The bubble has characteristic size ε>0, with its density and bulk modulus depending on the same small parameter through the Minnaert high-contrast scaling. The analysis is organized by the scaled separation Θε := dist(Dε,Γ)/ε, and covers the three natural regimes Θε→+∞, Θε→Θ*∈(0,∞), Θε→0: 1) In the far-separation regime, the interface is invisible at leading order and the classical full-space Minnaert law is recovered. 2) In the critical regime, the rescaled geometry retains both the bubble and the interface at finite separation, and the Newtonian capacitance is replaced by a flat-interface capacitance determined by the limiting tangent transmission problem. 3) In the near-contact regime, this family converges to a contact-limiting capacitance, yielding the same leading-order Minnaert resonance for all gap scalings satisfying dist(Dε,Γ) = o(ε). These three regimes provide a unified description of how the resonance frequency changes as the bubble approaches the interface, from the classical isolated-bubble limit to the contact limit. The analysis relies on a uniform reduction of the resonance problem to a scalar equation and on a variational characterization of the interface-dependent capacitances; in particular, Mosco convergence of the associated transmission energies yields convergence of the capacitary potentials and minimum energies up to the singular contact configuration.

Related

  1. Forward-Backward McKean-Vlasov System with Jumps and a Monotone Source With à Control-Shifted Interface : Well-Posedness, Stability, and Yosida Rates
    Kayembe Tshiswaka Tcheick, Mabela Matendo Rostin, Kabengele Mpunga Yannick +1
    arXivPreprintarXiv licenceFull textOptimisation & controlarXiv
  2. Shifted wave equation on noncompact symmetric spaces
    Yulia Kuznetsova, Zhipeng Song
    HALPreprintLicence not statedFull textGeneral mathematicsHAL
  3. Shifted Composition III: Local Error Framework for KL Divergence
    Jason M. Altschuler, Sinho Chewi
    Foundations of Computational MathematicsPeer-reviewedLicence not statedFull text19 citedStatisticsOpenAlex
  4. Quivers with Involutions and Shifted Twisted Yangians via Coulomb Branches
    Yaolong Shen, Changjian Su, Rui Xiong
    Communications in Mathematical PhysicsPeer-reviewedLicence not statedFull text14 citedGeometry & topologyOpenAlex
  5. Shifted convolutions of divisor functions
    Miguel N. Walsh
    arXivPreprintarXiv licenceFull textAlgebra & number theoryarXiv
BibTeX
@misc{diao2026interfaceshifted,
  title = {{Interface-Shifted Minnaert Resonances}},
  author = {Huaian Diao and Long Li and Mourad Sini},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.37423},
  eprint = {2609.37423},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.37423},
}
RIS
TY  - UNPB
TI  - Interface-Shifted Minnaert Resonances
AU  - Huaian Diao
AU  - Long Li
AU  - Mourad Sini
PY  - 2026
DA  - 2026/09/29
PB  - arXiv
DO  - 10.48550/arxiv.2609.37423
UR  - https://arxiv.org/abs/2609.37423
AB  - We develop a unified asymptotic theory for Minnaert resonances generated by a small bubble D_ε placed near an interface Γ of material discontinuity in an acoustic background. The bubble has characteristic size ε>0, with its density and bulk modulus depending on the same small parameter through the Minnaert high-contrast scaling. The analysis is organized by the scaled separation Θ_ε := dist(D_ε,Γ)/ε, and covers the three natural regimes Θ_ε→+∞, Θ_ε→Θ_*∈(0,∞), Θ_ε→0: 1) In the far-separation regime, the interface is invisible at leading order and the classical full-space Minnaert law is recovered. 2) In the critical regime, the rescaled geometry retains both the bubble and the interface at finite separation, and the Newtonian capacitance is replaced by a flat-interface capacitance determined by the limiting tangent transmission problem. 3) In the near-contact regime, this family converges to a contact-limiting capacitance, yielding the same leading-order Minnaert resonance for all gap scalings satisfying dist(D_ε,Γ) = o(ε). These three regimes provide a unified description of how the resonance frequency changes as the bubble approaches the interface, from the classical isolated-bubble limit to the contact limit. The analysis relies on a uniform reduction of the resonance problem to a scalar equation and on a variational characterization of the interface-dependent capacitances; in particular, Mosco convergence of the associated transmission energies yields convergence of the capacitary potentials and minimum energies up to the singular contact configuration.
ER  -