2017
DOI: 10.1007/978-3-319-52389-7_32
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SHEM: An Optimal Coarse Space for RAS and Its Multiscale Approximation

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Cited by 24 publications
(34 citation statements)
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“…While there is currently no practical realization of this algorithm, the fact that the algorithm converges in two iterations, independently of the number of subdomains, suggests that a coarse space component is active in this optimal algorithm. Coarse spaces leading to nilpotent iterations have first been described in the lecture notes [68], and then in [70,71], with successful approximations in [74,75]. The property of domain decomposition methods in general to be nilpotent has only very recently been investigated in more detail, see [24].…”
Section: Discussionmentioning
confidence: 99%
“…While there is currently no practical realization of this algorithm, the fact that the algorithm converges in two iterations, independently of the number of subdomains, suggests that a coarse space component is active in this optimal algorithm. Coarse spaces leading to nilpotent iterations have first been described in the lecture notes [68], and then in [70,71], with successful approximations in [74,75]. The property of domain decomposition methods in general to be nilpotent has only very recently been investigated in more detail, see [24].…”
Section: Discussionmentioning
confidence: 99%
“…Notice that the dimension of V N c is proportional to N . It is clear that the coarse space V N c has mainly information condensed on the boundaries of the objects, similar to the Spectral Harmonically Enriched Multiscale coarse space SHEM in domain decomposition [21,20], which contains mainly information on the interfaces between subdomains, see also [19,18]. It is important to remark that the construction of each function ϕ j,n would require the solution of problem (6.1), which requires the same computational effort of the original problem (2.3).…”
Section: Scalability Analysis and Coarse Correctionmentioning
confidence: 99%
“…The basis functions are obtained by solving local problems mimicking (1) at the scale of mesh elements, with carefully chosen right-hand sides and boundary conditions. The vanilla version of the approach, called linear MsFEM, uses as basis functions the solutions to these local problems, posed on each mesh element, with null right-hand sides and with the coarse P1 elements as Dirichlet boundary conditions (see (12) below for the precise definition of these basis functions). Various improvements of that version are possible.…”
Section: Introductionmentioning
confidence: 99%