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Radiating and non-radiating sources in elasticity
Analysis of PDEs · Submitted 19 Jul 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim If the support of such a force has a convex or non-convex corner or edge on their boundary, the force must be vanishing there.
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The abstract, sentence by sentence
In this work, we study the inverse source problem of a fixed frequency for the Navier's equation. We investigate that nonradiating external forces. If the support of such a force has a convex or non-convex corner or edge on their boundary, the force must be vanishing there. The vanishing property at corners and edges holds also for sufficiently smooth transmission eigenfunctions in elasticity. The idea originates from the enclosure method: The energy identity and new type exponential solutions for the Navier's equation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this work, we study the inverse source problem of a fixed frequency for the Navier's equation. | contribution 0.78 | 0.81 | 0.04 | asserted 0.79 |
| s1 | We investigate that nonradiating external forces. | contribution 0.98 | 0.80 | 0.07 | unclear 0.58 |
| s2 | If the support of such a force has a convex or non-convex corner or edge on their boundary, the force must be vanishing there. | result 1.00 | 0.79 | 0.58 | asserted 1.00 |
| s3 | The vanishing property at corners and edges holds also for sufficiently smooth transmission eigenfunctions in elasticity. | result 0.97 | 0.68 | 0.16 | asserted 0.99 |
| s4 | The idea originates from the enclosure method: The energy identity and new type exponential solutions for the Navier's equation. | method 0.97 | 0.28 | 0.03 | asserted 0.98 |
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Original abstract
In this work, we study the inverse source problem of a fixed frequency for the Navier's equation. We investigate that nonradiating external forces. If the support of such a force has a convex or non-convex corner or edge on their boundary, the force must be vanishing there. The vanishing property at corners and edges holds also for sufficiently smooth transmission eigenfunctions in elasticity. The idea originates from the enclosure method: The energy identity and new type exponential solutions for the Navier's equation.
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Furthermore, in a slightly different context, the Schiffer's problem was studied in a nonlocal setup, see [ref] .
Simultaneously recovering potentials and embedded obstacles for anisotropic fractional Schr\"odinger operators · Motivation and background · 0.89
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