Abstract

This paper concerns the transmission eigenvalue problem for an inhomogeneous media of compact support containing small penetrable homogeneous inclusions. Assuming that the inhomogeneous background media is known and smooth, we investigate how these small volume inclusions affect the real transmission eigenvalues. Note that for practical applications the real transmission eigenvalues are important since they can be measured from the scattering data. In particular, in addition to proving the convergence rate for the eigenvalues corresponding to the perturbed media as inclusions' volume goes to zero, we also provide the explicit first correction term in the asymptotic expansion for simple eigenvalues. The correction terms involves the eigenvalues and eigenvectors of the unperturbed known background as well as information about the location, size and refractive index of small inhomogeneities. Thus, our asymptotic formula has the potential to be used to recover information about small inclusions from a knowledge of real transmission eigenvalues.

Highlights

  • The transmission eigenvalue problem, which is a non-selfadjoint and non-linear eigenvalue problem, appears in the study of the scattering problem for inhomogeneous media [7]

  • The corresponding transmission eigenvalues can be determined from the scattering data [3], [13] and provide information about material properties of the scattering media [4], [5]

  • The transmission eigenvalue problem is a non-selfadjoint and nonlinear problem that is not covered by the standard theory of eigenvalue problems for elliptic operators

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Summary

Introduction

The transmission eigenvalue problem, which is a non-selfadjoint and non-linear eigenvalue problem, appears in the study of the scattering problem for inhomogeneous media [7]. In the current paper the transmission eigenvalue problem is written as a non-linear eigenvalue problem for a compact operator following the fourth order formulation approach developed in [6] and [5]. This approach restricts us to study the perturbation of only real eigenvalues, which from practical application point of view is sufficient since the real eigenvalues are measurable from the scattering data.

Inverse Problems and Imaging
Ciτ i for
We begin by considering
We calculate
Recall that by assumption we have
Ci τ i
Let us choose φ
Because u
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