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Additive Schwarz condition bound from stable decomposition and synthesis

Statement

Use the data of Finite-dimensional Schwarz subspace-correction data and assume the local spaces span V. Suppose 0<C0,C1<∞ satisfy:

  • for every x∈V, there are local vectors zi such that x=∑iRizi and ∑iziTAizi≤C0∥x∥A2;
  • for every tuple (zi), ∥∑iRizi∥A2≤C1∑iziTAizi.

For an A-self-adjoint positive operator T, define λmin⁡A(T)=inf⁡x≠0a(Tx,x)a(x,x),λmax⁡A(T)=sup⁡x≠0a(Tx,x)a(x,x),κA(T)=λmax⁡A(T)λmin⁡A(T). Then the exact additive Schwarz operator T=BA is A-self-adjoint positive and λmin⁡A(BA)≥C0−1,λmax⁡A(BA)≤C1,κA(BA)≤C0C1. If the inexact local matrices satisfy αAi⪯A~i⪯βAi for 0<α≤β, then λmin⁡A(B~A)≥(βC0)−1,λmax⁡A(B~A)≤C1/α,κA(B~A)≤(β/α)C0C1.

Facts & Assumptions

Given: The real SPD matrix A, the prolongations Ri, stable-decomposition constant C0, synthesis constant C1, and, for the inexact branch, uniform local spectral-equivalence constants α,β.

[F1]

The exact additive preconditioner is B=∑iRiAi−1RiT, with Πi=RiAi−1RiTA and BA=∑iΠi (Finite-dimensional Schwarz subspace-correction data).

[F2]

Each Πi is an A-orthogonal projection and a(Πix,x)=∥Πix∥A2 (Exact Schwarz local corrections are energy-orthogonal projections).

[F3]

If the local spaces span V, B is SPD and xTB−1x is the minimum summed local energy over decompositions (The additive Schwarz inverse minimizes summed local energy).

[F4]

The exact local matrices Ai are SPD (Schwarz local matrices and exact solves are well defined).

[F5]

In every real inner-product space, ∣a(u,v)∣≤∥u∥A∥v∥A (Cauchy–Schwarz: ∣⟨x,y⟩∣≤∥x∥ ∥y∥, with equality exactly for dependent pairs).

Proof

1.1F1F2F3given

The stable-decomposition hypothesis implies that the local spaces span V, so [F3] makes B SPD. Each Πi is A-self-adjoint by [F2], hence T=BA=∑iΠi is A-self-adjoint. Moreover a(Tx,x)=∑i∥Πix∥A2≥0; if this is zero, then every Πix=0. For any vi∈Vi, [F2] gives Πivi=vi, so a(x,vi)=a(Πix,vi)=0. The spaces span V, hence x=0 and T is positive.

1.2F1F2F5givenalgebra

Fix x≠0 and choose the decomposition x=∑iRizi from the stable-decomposition hypothesis. Orthogonal projection gives ∥x∥A2=∑ia(x,Rizi)=∑ia(Πix,Rizi)≤(∑i∥Πix∥A2)1/2(∑iziTAizi)1/2. The last inequality is [F5] in the product inner product on the finite tuple space. The assumed bound on the second factor yields a(Tx,x)=∑i∥Πix∥A2≥C0−1∥x∥A2, proving the lower Rayleigh bound.

1.3F1F2F5givenalgebra

For each x, write Πix=Riyi with yi=Ai−1RiTAx. The synthesis hypothesis and [F2] give ∥Tx∥A2=∥∑iRiyi∥A2≤C1∑i∥Πix∥A2=C1a(Tx,x). Set q=a(Tx,x)/∥x∥A2. [F5] gives q∥x∥A≤∥Tx∥A, while the displayed inequality gives ∥Tx∥A2≤C1q∥x∥A2. If q>0, these imply q≤C1; if q=0, the same upper bound is immediate.

1.4F4givenalgebra

By [F4] and the assumed lower order bound, every A~i is SPD. For every SPD matrix M and vector y, yTM−1y=max⁡z(2yTz−zTMz), because completing the square subtracts (z−M−1y)TM(z−M−1y). Since A~i⪯βAi, this maximum for A~i is at least the maximum for βAi, namely β−1yTAi−1y; since αAi⪯A~i, it is at most the maximum for αAi, namely α−1yTAi−1y. Thus β−1Ai−1⪯A~i−1⪯α−1Ai−1. Summing after congruence by Ri yields β−1B⪯B~⪯α−1B.

2.1givenstep 1.1step 1.2step 1.3step 1.4algebra∎

Step 1.4 establishes that each inverse in B~ is SPD. By the stable-decomposition hypothesis, the local spaces span V; hence if x≠0 then RiTx≠0 for some i, since otherwise x would be Euclidean-orthogonal to their span V. Therefore xTB~x=∑i(RiTx)TA~i−1(RiTx)>0, so B~ is symmetric positive definite. It follows that B~A is A-self-adjoint and positive, because AB~A is symmetric positive definite; the inexact Rayleigh quotient and condition number are therefore defined. The matrix comparison in step 1.4 bounds a(B~Ax,x)=xTAB~Ax below by β−1xTABAx and above by α−1xTABAx. The exact bounds in steps 1.2 and 1.3 therefore give the stated inexact minimum, maximum, and condition-ratio bounds.

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