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        <h2>Section: 
      Research Program</h2>
        <h3 class="titre3">Multiphysics coupling and
domain decomposition</h3>
        <p>Within our project, we start from the
conception and analysis of <i>models</i> based on <i>partial
differential equations</i>. Already at the PDE level, we address the
question of <i>coupling</i> of different models; examples may be that
of simultaneous fluid flow in a discrete network of two-dimensional
<i>fractures</i> and in the surrounding three-dimensional porous
medium, or that of interaction of a compressible flow with the
surrounding elastic deformable structure. The key physical
characteristics need to be captured, whereas existence, uniqueness,
and continuous dependence on the data are minimal analytic
requirements that we request to satisfy. At the modeling stage, we
also plan to develop model-order reduction techniques, such as the
use of reduced basis techniques or proper generalized decompositions,
to tackle evolutive problems, in particular in the nonlinear case.</p>
        <p>We also concentrate an important effort on the development and
analysis of efficient solvers for the systems of nonlinear algebraic
equations. We have already in the past developed <i>Newton–Krylov
solvers</i>, with a particular impact on <i>parallelization</i> that we
achieve via <i>domain decomposition</i>. Here we specialize on Robin
boundary conditions, where an optimized choice of the parameter has
already shown speed-ups in orders of magnitude in terms of the number
of the iterations of the domain decomposition algorithm in question.
A novel feature is the use of such algorithms in time-dependent
problems in <i>space-time</i> domain decomposition which allows the
use of different time steps in different parts of the computational
domain. This is particularly useful in porous media applications,
where the amount of diffusion (permeability) varies abruptly, so that
the evolution speeds vary importantly and call for adapted localized
time stepping. Our other novel theme are <i>Newton–multigrid
solvers</i>, where the geometric multigrid solver ingredients are <i>tailored</i> to the specific problem under consideration and to the
specific numerical method, with problem- and discretization-dependent
restriction, prolongation, and smoothing. This in particular yields
<i>mass balance</i> on <i>each iteration step</i>, a very welcome
feature in most of the target applications. The solver itself is then
<i>steered adaptively</i> at each execution step by an a posteriori
error estimate.
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