2013
DOI: 10.1002/nla.1869
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Hierarchical Schur complement preconditioner for the stochastic Galerkin finite element methods

Abstract: Use of the stochastic Galerkin finite element methods leads to large systems of linear equations obtained by the discretization of tensor product solution spaces along their spatial and stochastic dimensions. These systems are typically solved iteratively by a Krylov subspace method. We propose a preconditioner, which takes an advantage of the recursive hierarchy in the structure of the global matrices. In particular, the matrices posses a recursive hierarchical two-by-two structure, with one of the submatrice… Show more

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Cited by 41 publications
(40 citation statements)
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“…, s K − 1, we can use the splitting U = V TP s 1 ,...,s K−1 ,s K −1 and W such that V TP s 1 ,...,s K = U ⊕ W , i.e., W contains the polynomials of V TP s 1 ,...,s K of degree exactly s K − 1 in the variable ξ K . The corresponding preconditioning matrix M has then a two-by-two block-diagonal form, see, e.g., [30,32], and can be obtained as…”
Section: 3mentioning
confidence: 99%
“…, s K − 1, we can use the splitting U = V TP s 1 ,...,s K−1 ,s K −1 and W such that V TP s 1 ,...,s K = U ⊕ W , i.e., W contains the polynomials of V TP s 1 ,...,s K of degree exactly s K − 1 in the variable ξ K . The corresponding preconditioning matrix M has then a two-by-two block-diagonal form, see, e.g., [30,32], and can be obtained as…”
Section: 3mentioning
confidence: 99%
“…Preconditioners that exploit the structure of A are another essential ingredient (see, for example, [17], [23], [22], [18], [8]). In particular, the mean-based preconditioner P = G 0 ⊗ K 0 analyzed by Powell & Elman in [17] requires n ξ inexact decoupled solves with K 0 in each CG iteration.…”
Section: 2)mentioning
confidence: 99%
“…To simplify exposition, we use the continuous block operator notation analogous to [40]. Given a consistent spatial discretization method, we write the discrete approximations of the continuous spatial operators in the deterministic PDE 1 and 2 as (27) G h p ≈ ∇ p, (28) D h u ≈ ∇ · u, (29) N h p ≈ ∇ 2 p, (30) I h p ≈ p. (31) In contrast to the deterministic case, we modify matrices for the stochastic system (13) and (14) by enforcing all zero rows corresponding to boundary nodes in operators (26)- (31). The polynomial chaos coefficients defined in (15)-(17) and (18) and (19) also form matrices of size P × P denoted by , B, A, C, and K, respectively.…”
Section: Discretizationmentioning
confidence: 99%