2020
DOI: 10.1016/j.cma.2020.113406
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Adjoint-state method for Hybridizable Discontinuous Galerkin discretization, application to the inverse acoustic wave problem

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Cited by 14 publications
(22 citation statements)
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“…Our FWI-based reconstruction uses an iterative Newton-type method on an L 2 distance between data and simulations. For the discretization of the resulting partial differential equations, we use the hybridizable discontinuous Galerkin method (HDG), [8,18], and the open-source parallel software hawen 1 , [14].…”
Section: Contribution and Outlinementioning
confidence: 99%
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“…Our FWI-based reconstruction uses an iterative Newton-type method on an L 2 distance between data and simulations. For the discretization of the resulting partial differential equations, we use the hybridizable discontinuous Galerkin method (HDG), [8,18], and the open-source parallel software hawen 1 , [14].…”
Section: Contribution and Outlinementioning
confidence: 99%
“…In this section, we numerically compare the forward models presented above. For the discretization of the partial differential equation, we use the hybridizable discontinuous Galerkin method (HDG), [8,18], and the open-source parallel software hawen, see [14] and footnote 1. It is further employed to carry out the reconstruction with FWI in Section 6.1.…”
Section: Numerical Comparison Of Forward Modelsmentioning
confidence: 99%
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“…The HDG method is specifically designed for first-order problems as it allows to maintain a small linear system compared to other discretizations, as observed by, e.g., [13,22,10,15]. The implementation follows two levels with first the global system for the numerical trace and then local systems for the volume solution.…”
Section: Numerical Calculation Of the Green's Functionmentioning
confidence: 99%
“…Figure 12 shows the time-distance diagram for C surf (θ, t) where θ =r 1 •r 2 is the angle between the two observation points 648r 1 andr 2 . We first compute C surf (θ, ω) using (4.18) with a frequency h ω = 5 µHz and then apply the inverse Fourier transform using (4.19) with N t = 2 15 . We show the section at θ = 30 • for the different RBC, together with the difference with respect to the reference (using Z DtN ) solution.…”
Section: Radiation Boundary Conditions For Time-distance Diagrammentioning
confidence: 99%