2006
DOI: 10.1364/ao.45.002828
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Dynamically adaptive mesh refinement technique for image reconstruction in optical tomography

Abstract: A novel adaptive mesh technique is introduced for problems of image reconstruction in luminescence optical tomography. A dynamical adaptation of the three-dimensional scheme based on the finite-volume formulation reduces computational time and balances the ill-posed nature of the inverse problem. The arbitrary shape of the bounding surface is handled by an additional refinement of computational cells on the boundary. Dynamical shrinking of the search volume is introduced to improve computational performance an… Show more

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Cited by 17 publications
(15 citation statements)
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“…29 for an overview of the different models͒. Although general models such as the telegraph equation 30 or the radiative transfer equation 31 can be used, the light propagation in FDOT is classically assumed to follow the diffusion equation. Within this framework, the photon density ͒ is the source term.…”
Section: Iia1 Light Propagationmentioning
confidence: 99%
“…29 for an overview of the different models͒. Although general models such as the telegraph equation 30 or the radiative transfer equation 31 can be used, the light propagation in FDOT is classically assumed to follow the diffusion equation. Within this framework, the photon density ͒ is the source term.…”
Section: Iia1 Light Propagationmentioning
confidence: 99%
“…The system of Eq. (26) is further discretized and solved numerically in the Fourier domain on the adaptive Cartesian grid [15,24] by use of the conjugate gradient method with early termination of the iterative process, which has a regularization effect. The number of iterations is found empirically from the discrepancy principle [25].…”
Section: Inverse Problem: the Time Domain Versus The Fourier Domainmentioning
confidence: 99%
“…The solution of this system is used for iterative reconstruction of optical and fluorescent parameters. Equations are solved on a Cartesian mesh by utilizing the Finite Volume numerical scheme [25,26] and the ray tracing technique [27]. Although in our experimental setup relative positions of the laser source and the CCD camera are fixed, while the object under study is rotated, computationally we rotate source positions and the CCD camera in the opposite direction.…”
Section: B Inverse Problem: Variational Frameworkmentioning
confidence: 99%
“…In the reconstruction algorithm Eqs. (23)(24)(25)(26) are replaced with two Helmholtz equations for adjoint average integrated intensities, ψ and ψ′, [19] and all terms containing I, I′, J and J′ are dropped in Eqs. (28)(29)(30)(31).…”
Section: A the Telegraph Equation Approximationmentioning
confidence: 99%