1995
DOI: 10.1117/12.209991
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<title>Image reconstruction for random media by diffusion tomography</title>

Abstract: As mathematical model for the light propagation in highly scattering media the diffusion equation for the photon density is used. The solution of the forward problem obtained by the Finite Element Method (FEM) is compared with the analytical solution in a rectangle homogeneous domain. The application of a numerical method as the FEM allows to take into account different geometries and various embedded objects. For the inverse imaging problem two reconstruction methods are introduced acting as iterative algorit… Show more

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Cited by 3 publications
(3 citation statements)
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“…162 have been reported by several groups. [33][34][35][36][37][38][39] If the voxel dimensions are larger than the diffusion coefficient D1r2-and preferably several times that-and the boundary conditions are properly chosen, the performance of a diffusion-based imaging operator can be qualitatively very similar to that of the transport-based operator. Unfortunately, there is as yet no set of standardized problems on which all groups work, so no detailed quantitative comparison of different approaches to either the forward or the inverse problem is possible.…”
Section: Discussionmentioning
confidence: 99%
“…162 have been reported by several groups. [33][34][35][36][37][38][39] If the voxel dimensions are larger than the diffusion coefficient D1r2-and preferably several times that-and the boundary conditions are properly chosen, the performance of a diffusion-based imaging operator can be qualitatively very similar to that of the transport-based operator. Unfortunately, there is as yet no set of standardized problems on which all groups work, so no detailed quantitative comparison of different approaches to either the forward or the inverse problem is possible.…”
Section: Discussionmentioning
confidence: 99%
“…The light propagation in highly scattering media may be described by the widely used diffusion approximation of the Boltzmann transport equation, which leads to the parabolic differential equation for the photon density ' (1) Here c is the speed of light in the medium, pa(X) the absorption coefficient and s(x, t) a source term. The optical diffusion coefficient is…”
Section: Mathematical Modelmentioning
confidence: 99%
“…For completeness, an initial condition (x, 0) = O(x) must be given. The light source may be described in two ways, first by the photon source term s(x, t) in equation(1) and secondly by the initial function 0(x) corresponding to a 5-pulse in time. For short light pulses, as considered here, the results are approximately the same.…”
mentioning
confidence: 99%