Journal
SIAM JOURNAL ON MATHEMATICAL ANALYSIS
Volume 54, Issue 5, Pages 5160-5181Publisher
SIAM PUBLICATIONS
DOI: 10.1137/21M1463689
Keywords
inverse source problem; asymptotic expansion; Riesz basis
Categories
Funding
- National Natural Science Foundation of China [12071072, 11971104]
- Austrian Science Fund (FWF) [P 30756-NBL]
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This study proposes a novel approach to recover an unknown source by measuring the wave fields generated by injecting small particles into the medium. By deriving the asymptotic expansion of the wave field and utilizing Riesz theory, the source term was successfully reconstructed.
The inverse problem of reconstructing a source term from boundary measurements, for the wave equation, is revisited. We propose a novel approach to recover the unknown source through measuring the wave fields after injecting small particles, enjoying a high contrast, into the medium. For this purpose, we first derive the asymptotic expansion of the wave field, based on the time-domain Lippmann-Schwinger equation. The dominant term in the asymptotic expansion is expressed as an infinite series in terms of the eigenvalues {\lambdan}n\in\BbbN of the Newtonian operator (for the pure Laplacian). Such expansions are useful under a certain scale between the size of the particles and their contrast. Second, we observe that the relevant eigenvalues appearing in the expansion have non-zero averaged eigenfunctions. We prove that the family {sin( c1/root lambda n t), cos( c1/root lambda n t)}, for those relevant eigenvalues, with c1 as the contrast of the small particle, defines a Riesz basis (contrary to the family corresponding to the whole sequence of eigenvalues). Then, using the Riesz theory, we reconstruct the wave field, generated before injecting the particles, on the center of the particles. Finally, from internal values of the last field, we reconstruct the source term by numerical differentiation, for instance. A significant advantage of our approach is that we only need the measurements on {x} \times (0, T) for a single point x away from \Omega , i.e., the support of the source, and large enough T.
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