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Elastic Calderón Problem via Resonant Hard Inclusions: Linearisation of the N-D Map and Density Reconstruction

Huaian Diao, Mourad Sini, Ruixiang Tang

TL;DR

This work addresses the elastic Calderón problem of recovering a spatial density ρ from boundary Neumann-to-Dirichlet data for the time-harmonic Lamé system. By embedding a subwavelength periodic cluster of resonant hard inclusions, the authors create an effective medium with a uniform negative density shift, enabling a near-linear relationship between the N--D map and the unknown density around a negative background. They establish a quantitative convergence Λ_D → Λ_P, derive a first-order linearisation around the background, and, using complex geometric optics solutions, obtain an explicit Fourier-reconstruction formula for ρ with controlled error. The results provide a metamaterial-inspired, analytically tractable framework for elastic inverse problems and a concrete approach for density reconstruction via nanoscale resonators.

Abstract

We study an elastic Calderon-type inverse problem: recover the mass density $ρ(x)$ in a bounded domain $Ω\subset\mathbb{R}^3$ from the Neumann-to-Dirichlet map associated with the isotropic Lamé system $\mathcal{L}_{λ,μ}u+ω^2ρ(x)u=0$. We introduce a constructive strategy that embeds a subwavelength periodic array of resonant high-density (hard) inclusions to create an effective medium with a uniform negative density shift. Specifically, we place a periodic cluster of inclusions of size $a$ and density $ρ_1\asymp a^{-2}$ strictly inside $Ω$. For frequencies $ω$ tuned to an eigenvalue of the elastic Newton (Kelvin) operator of a single inclusion, we show that as $a\to0$ and the number of inclusions $M\to\infty$, the Neumann-to-Dirichlet map $Λ_D$ converges to an effective map $Λ_{\mathcal{P}}$ corresponding to a background density shift $-\mathcal{P}^2$, with the operator norm estimate $\|Λ_D-Λ_{\mathcal{P}}\|\le Ca^α\mathcal{P}^6$ for some $α>0$ determined by the geometric scaling. Around this negative background we derive a first-order linearization of $Λ_{\mathcal{P}}$ in terms of $ρ$ and the Newton volume potential for the shifted Lamé operator. Testing the linearized relation with complex geometric optics solutions yields an explicit reconstruction formula for the Fourier transform of $ρ$, and hence a global density recovery scheme. The results provide a metamaterial-inspired analytic framework for inverse coefficient problems in linear elasticity and a concrete paradigm for leveraging nanoscale resonators in reconstruction algorithms.

Elastic Calderón Problem via Resonant Hard Inclusions: Linearisation of the N-D Map and Density Reconstruction

TL;DR

This work addresses the elastic Calderón problem of recovering a spatial density ρ from boundary Neumann-to-Dirichlet data for the time-harmonic Lamé system. By embedding a subwavelength periodic cluster of resonant hard inclusions, the authors create an effective medium with a uniform negative density shift, enabling a near-linear relationship between the N--D map and the unknown density around a negative background. They establish a quantitative convergence Λ_D → Λ_P, derive a first-order linearisation around the background, and, using complex geometric optics solutions, obtain an explicit Fourier-reconstruction formula for ρ with controlled error. The results provide a metamaterial-inspired, analytically tractable framework for elastic inverse problems and a concrete approach for density reconstruction via nanoscale resonators.

Abstract

We study an elastic Calderon-type inverse problem: recover the mass density in a bounded domain from the Neumann-to-Dirichlet map associated with the isotropic Lamé system . We introduce a constructive strategy that embeds a subwavelength periodic array of resonant high-density (hard) inclusions to create an effective medium with a uniform negative density shift. Specifically, we place a periodic cluster of inclusions of size and density strictly inside . For frequencies tuned to an eigenvalue of the elastic Newton (Kelvin) operator of a single inclusion, we show that as and the number of inclusions , the Neumann-to-Dirichlet map converges to an effective map corresponding to a background density shift , with the operator norm estimate for some determined by the geometric scaling. Around this negative background we derive a first-order linearization of in terms of and the Newton volume potential for the shifted Lamé operator. Testing the linearized relation with complex geometric optics solutions yields an explicit reconstruction formula for the Fourier transform of , and hence a global density recovery scheme. The results provide a metamaterial-inspired analytic framework for inverse coefficient problems in linear elasticity and a concrete paradigm for leveraging nanoscale resonators in reconstruction algorithms.
Paper Structure (25 sections, 14 theorems, 416 equations, 2 figures)

This paper contains 25 sections, 14 theorems, 416 equations, 2 figures.

Key Result

Theorem 1.1

Assume that the domain $\Omega$ is $C^{2}$-smooth. Let the density $\rho(\mathbf{x})$ satisfy $\rho(\cdot)\in \mathbb{W}^{1,\infty}(\Omega)$, and suppose the operating frequency $\omega$ meets the condition eq:the angular frequency. Choose a parameter $h$ with $\frac{1}{3}<h<1$, and assume that the uniformly for $(\mathbf{f},\mathbf{g})\in \mathbb{H}^{-1/2}(\partial\Omega)\times \mathbb{H}^{-1/2}

Figures (2)

  • Figure 1: An illustration of how the hard inclusion are distributed in $\Omega$.
  • Figure 2: Flow Chart of the proof strategy of Theorem \ref{['thm:N--D']}

Theorems & Definitions (29)

  • Theorem 1.1
  • Remark 1.1
  • Theorem 1.2
  • Theorem 1.3
  • Remark 1.2
  • Remark 1.3
  • Lemma 2.1
  • proof
  • Lemma 2.2
  • proof
  • ...and 19 more