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Cea transfers the fixed-mesh analytic p rate to the energy error

Statement

Assume Countable Choice. On a fixed finite matching affine tensor-box mesh, let V=H1(Ω) with its standard norm, let a(v,w)=∫Ω(∇v⋅∇w+vw), and let F be a bounded linear functional on V. Let u∈V solve a(u,w)=F(w) for all w∈V, and let up be its conforming Galerkin solution in the common-degree trace-matching tensor space of Variable-degree conforming hp spaces on matching affine meshes. If the analytic hypotheses of Analytic data converge exponentially under fixed-mesh p refinement hold with constants M,R and R−1<q<1, then

∥u−up∥H1(Ω)≤CT,d,R,qMqp.

This is the fixed-mesh analytic branch; it does not assert an h-dependent estimate or an ordinary Sobolev p-rate on simplices.

Facts & Assumptions

Given: Countable Choice; the finite matching affine tensor mesh; a,F,u,V as in the Statement; integer p≥1; and the analytic derivative bound and q of the fixed-mesh projector theorem.

[F1]

Matching variable-degree polynomial traces give an H1 function: the trace-matching tensor space is a finite-dimensional subspace of H1(Ω).

[F2]

Analytic data converge exponentially under fixed-mesh p refinement: there is a trace-matching up∗∈Vp with ∥u−up∗∥H1≤CT,d,R,qMqp.

[F3]

Céa quasi-optimality for coercive conforming Galerkin problems: under Countable Choice, a bounded coercive form on a Hilbert space and a finite-dimensional conforming subspace have a Galerkin solution satisfying ∥u−up∥V≤(Ma/αa)inf⁡vp∈Vp∥u−vp∥V.

[A1]

For the form in the Statement, Cauchy–Schwarz gives ∣a(v,w)∣≤∥v∥H1∥w∥H1 and a(v,v)=∥v∥H12.

Proof

1.1A1F1F3given

By [F1], Vp is finite-dimensional and contained in the Hilbert space V. The form in [A1] is bounded with Ma=1 and coercive with αa=1. The exact solution and bounded functional are among the hypotheses in Given, so [F3] applies and yields ∥u−up∥H1≤inf⁡vp∈Vp∥u−vp∥H1. Its only axiom beyond classical real analysis is Countable Choice, stated in Given.

2.1F2step 1.1algebra∎

The approximant up∗ in [F2] belongs to Vp, so the infimum in step 1.1 is no greater than ∥u−up∗∥H1. Substituting its bound from [F2] proves the stated energy estimate.

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