2014
DOI: 10.1137/130931291
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Reconstruction of a Conformally Euclidean Metric from Local Boundary Diffraction Travel Times

Abstract: Abstract. We consider a region M in R n with boundary ∂M and a metric g on M conformal to the Euclidean metric. We analyze the inverse problem, originally formulated by Dix [9], of reconstructing g from boundary measurements associated with the single scattering of seismic waves in this region. In our formulation the measurements determine the shape operator of wavefronts outside of M originating at diffraction points within M . We develop an explicit reconstruction procedure which consists of two steps. In th… Show more

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Cited by 15 publications
(18 citation statements)
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References 16 publications
(26 reference statements)
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“…In the case when the wave speed is isotropic, it is possible to transform the reconstruction from the travel time coordinates to the Euclidean coordinates. This transformation is considered in [6]. We also note that as an intermediate step in the proof of Theorem 2, we show that the metric can be recovered from S U locally in Fermi coordinates along geodesics passing through U .…”
Section: Theorem 2 Let M and M Be Two Smooth (Compact Or Complete) Rmentioning
confidence: 73%
See 1 more Smart Citation
“…In the case when the wave speed is isotropic, it is possible to transform the reconstruction from the travel time coordinates to the Euclidean coordinates. This transformation is considered in [6]. We also note that as an intermediate step in the proof of Theorem 2, we show that the metric can be recovered from S U locally in Fermi coordinates along geodesics passing through U .…”
Section: Theorem 2 Let M and M Be Two Smooth (Compact Or Complete) Rmentioning
confidence: 73%
“…Note that at the point γ x,η (r) we have ∂ r =γ x,η (r). Let r k j (r) = r k j (x, η, r) be the coefficients defined in (6), that is,…”
Section: Jacobi and Riccati Equationsmentioning
confidence: 99%
“…Which completes the demonstration of (14). Notice that we only require Λf | R , since, for t ∈ [0, T ], Λf (t) vanishes outside of R by finite speed of propagation.…”
Section: 2mentioning
confidence: 62%
“…In [5] a special case of problem [6] is considered. The authors study a setup where M ⊂ R n , n ≥ 2 and the metric tensor g| M = v −2 e, for some smooth and strictly positive function v. Let x ∈ R n \ M and y := γ x,ξ (t 0 ) ∈ M , for some ξ ∈ S x N and t 0 > 0, such that y is not a conjugate point to x along γ p,ξ .…”
Section: 23mentioning
confidence: 99%
“…The authors study a setup where M ⊂ R n , n ≥ 2 and the metric tensor g| M = v −2 e, for some smooth and strictly positive function v. Let x ∈ R n \ M and y := γ x,ξ (t 0 ) ∈ M , for some ξ ∈ S x N and t 0 > 0, such that y is not a conjugate point to x along γ p,ξ . The main theorem of [5] is that, if the coefficient functions of the shape operators of generalized spheres Σ y,r,W are known in a neighborhood V of γ x,ξ ([0, t 0 )) and the wave speed v is known in (N \ M ) ∩ V , then the wave speed v can be determined in some neighborhood V ⊂ V of γ x,ξ ([0, t 0 ]).…”
Section: 23mentioning
confidence: 99%