2007
DOI: 10.1137/050640655
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MUSIC‐Type Electromagnetic Imaging of a Collection of Small Three‐Dimensional Inclusions

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Cited by 170 publications
(177 citation statements)
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“…The scalar case was recently considered in [13]. Our approach in this paper, combined with the ones in [7,8], opens also a door for a numerical and mathematical framework for optimal shape design of resonant nanoparticles and their superresolved imaging. The limit when t → 0 − is computed similarly and we find (4.8) for k = 0.…”
Section: Discussionmentioning
confidence: 99%
“…The scalar case was recently considered in [13]. Our approach in this paper, combined with the ones in [7,8], opens also a door for a numerical and mathematical framework for optimal shape design of resonant nanoparticles and their superresolved imaging. The limit when t → 0 − is computed similarly and we find (4.8) for k = 0.…”
Section: Discussionmentioning
confidence: 99%
“…Extensions of this formula to unbounded domains have been considered in [11,28], and reconstruction methods for the corresponding inverse scattering problem in unbounded domains have been studied in [2,28,29,[31][32][33]. Assuming that the diameter of the scatterers described by ρ n is small, these methods neglect the o(ρ n 3 ) term in (5.1) and describe the measured electromagnetic fields by the leading order term in this formula.…”
Section: Examples and Applicationsmentioning
confidence: 99%
“…The asymptotic formulas for diametrically small conductivity inhomogeneities and scatterers known so far form the foundation of several efficient reconstruction methods for inverse conductivity problems (see, e.g., Ammari, Moskow, and Vogelius [7], Ammari and Seo [8] or Brühl, Hanke, and Vogelius [17]) and inverse scattering problems for Maxwell's equations (see, e.g., Ammari et al [2], Iakovleva et al [33], Volkov [42], or [28,29,31,32]). In addition the general formula for electrostatic potentials from [18] has recently been used to investigate inverse conductivity problems for wires and tubes (see Beretta et al [13] or [30]).…”
Section: Introductionmentioning
confidence: 99%
“…Using the summation convention, the relation between the stress and the displacement given by (2) can by written simply as σ ij = C ijkl ε kl , where the summation is understood to be over the repeated indexes k and l. By defining the vectors s and e as s = σ 11 , σ 22 , σ 33 , σ 23 , σ 31 , σ 12 t , (4) we can write the following relationship between the six independent components of stress and strain tensors:…”
Section: Notation and Preliminariesmentioning
confidence: 99%