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A smooth FAS cycle converges locally under its actual derivative bounds

Statement

Let E:U→Rn be the actual exact-branch error map of one fixed FAS two-grid or recursive V/W cycle, with U⊆Rn open. Let u∗∈U be a fine root for which the selected smoothers and coarse branches fix u∗, so E(u∗)=u∗. Assume E is C1 on a neighborhood of the closed Euclidean ball K=B‾2(u∗,r)⊂U. Put q=∥DE(u∗)∥op, where for a linear map T the induced Euclidean operator norm is ∥T∥op:=sup⁡∥v∥2=1∥Tv∥2. Suppose q<1 and ∥DE(x)−DE(y)∥op≤L∥x−y∥2(x,y∈K) for some L≥0. If q+Lr/2<1, then E(K)⊆K and every iteration uk+1=E(uk) starting in K satisfies ∥uk−u∗∥2≤(q+Lr/2)k∥u0−u∗∥2. This is a local result for the derivative of the actual cycle; it supplies no global-start or mesh-independent rate unless q,L,r are verified uniformly.

Facts & Assumptions

Given: The exact-branch FAS cycle map E, an exact root u∗ fixed by the cycle, a closed convex ball K⊂U, q=∥DE(u∗)∥op<1, and the stated Lipschitz bound for DE.

[F1]

An exact fine root is fixed by the FAS V/W cycle: when the smoothers fix exact roots and the coarse solver selects the restricted root at zero defect, the exact-branch V/W FAS cycle fixes the fine root.

[F2]

Derivative of the exact-branch FAS two-grid cycle: for a C1 two-grid exact branch with invertible coarse Jacobian, the actual cycle derivative includes the pre-smoother, I−PDFH(Iu∗)−1RDFh(u∗), and the post-smoother.

[F3]

Vector Newton remainder under a Lipschitz Jacobian: for a C1 map on a convex set with L-Lipschitz derivative, the endpoint Taylor remainder is bounded by L∥x−x∗∥22/2.

Proof

technique · contraction
1.1F1F2given

In the two-grid case, [F2] identifies DE(u∗) as the derivative of the actual pre-smoother, implicit coarse-branch correction, and post-smoother composition. For a recursive V/W cycle, q in the hypotheses is the derivative norm of that full composed map.

1.2givenF1F3algebra

Fix x∈K and put e=x−u∗. Apply [F3] with its variables x=u∗ and x∗=x. Reversing the resulting difference and using E(u∗)=u∗ gives ∥E(x)−u∗−DE(u∗)e∥2≤L2∥e∥22. Thus, since ∥DE(u∗)∥op=q and ∥e∥2≤r, ∥E(x)−u∗∥2≤q∥e∥2+L2∥e∥22≤κ∥e∥2,κ:=q+Lr/2<1.

2.1step 1.2algebra

For x∈K, step 1.2 gives ∥E(x)−u∗∥2≤κ∥x−u∗∥2≤κr<r, so E(x)∈K. This proves invariance of the stated ball.

3.1step 1.2step 2.1algebra∎

For an iterate starting at u0∈K, invariance keeps every uk in K and step 1.2 gives ∥uk+1−u∗∥2≤κ∥uk−u∗∥2. Induction yields ∥uk−u∗∥2≤κk∥u0−u∗∥2; because 0≤κ<1, the right side tends to zero.

Remarks

For the two-grid exact-branch cycle, Derivative of the exact-branch FAS two-grid cycle gives the derivative to be checked. For a recursive V/W cycle, the bound must be checked for the complete composed cycle. The one-sided estimate toward u∗ does not assert a Banach contraction bound between every pair of points in K.

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