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Symmetric Nitsche L2 estimate under dual regularity and Nitsche approximation

Statement

Assume Countable Choice and the symmetric Nitsche setup of Symmetric and nonsymmetric Nitsche boundary forms and Nitsche consistency and energy quasi-optimality with penalty above the symmetric coercivity threshold. Let e:=u−uh1∈L2(Ω) and let ζe∈H01(Ω) solve the adjoint Poisson problem ∫Ω∇v⋅∇ζe dx=∫Ωve dx for every v∈H01(Ω). Assume its dual regularity bound [A1] ∥ζe∥H1+s(Ω)≤CR∥e∥L2(Ω),s∈(1/2,1], The proved interpolation theorem Zero-boundary fractional interpolation in the Nitsche comparison norm supplies zh:=Ih,0ζe∈Yh and a mesh-uniform constant CD with ∥ζe−zh∥#,h≤CDhsℓΩ1−s∥ζe∥H1+s(Ω),0<h≤ℓΩ:=diam⁡(Ω). Set C∂ as in Global boundary-flux estimate on a matching mesh and preserve the original constant M1:=2+C∂+γ0. Then ∥u−uh1∥L2(Ω)≤M1CDCRhsℓΩ1−s∥u−uh1∥#,h, where the all-comparison-space symmetric form bound with this same M1 is proved below. The dual elliptic regularity estimate remains an explicit PDE hypothesis. If, in addition, the general higher-order/local primal energy approximation hypothesis [A3] holds with exponent t>0, then ∥u−uh1∥L2(Ω)≤M1CDCRCθCIhsℓΩ1−s(∑K∈ThhK2t∥u∥H1+t(K)2)1/2. The primal branch retains its full exponent range and local broken-norm hypothesis; the zero-boundary P1 interpolation theorem supplies the dual approximation and does not replace that branch.

Facts & Assumptions

Given: Countable Choice; the symmetric weak-boundary problem and its energy orthogonality; e=u−uh1; the zero-trace adjoint solution ζe; its stated dual regularity; and the remaining primal approximation hypothesis only for the final conditional branch.

[F1]

The energy theorem gives ah1(e,wh)=0 for all wh∈Vh (Nitsche consistency and energy quasi-optimality).

[F2]

H01(Ω) is formed from W1,2(Ω) using the zero-trace closure convention (Integer-order Sobolev spaces and their norms, Zero-boundary Sobolev space as a norm closure), and with its usual norm is a Hilbert space (The Sobolev space H1 is a Hilbert space). The adjoint variational equation is well-posed for a bounded coercive form on a Hilbert space under Countable Choice (Well-posedness of the adjoint variational problem). On bounded Ω, the Poincare inequality controls the L2 part of the W1,2 norm of a zero-trace function by its first-derivative part (The Poincare inequality for zero-boundary Sobolev closures on domains bounded in one direction).

[F3]

Hs(K) is the restriction of Hs(Rd) with the quotient Bessel-potential norm, and the weighted Fourier norm maps H1+s(Rd) continuously into Hs(Rd) under each first derivative (Restriction Bessel-potential spaces on polyhedral domains, Real-order Bessel-potential completion H^s, Real-order H^s as weighted Fourier distributions).

[F4]

For s>1/2, a function in Hs(K) has a unique bounded L2 trace on each affine simplex facet (Fractional Bessel-potential traces on simplex facets).

[F5]

Every real function in H01(Ω) has zero L2 trace on each boundary facet (Zero facet traces of functions in H1_0 on an affine mesh).

[F6]

If v∈H1+s(Ω), −Δv=g∈L2(Ω) distributionally, and the cellwise normal derivatives have the stated fractional traces, the weak Green supplier gives the global Green identity and interior flux cancellation for every w∈H1(Ω) (Fractional weak Green identity and interior flux cancellation).

[F7]

The zero-boundary fractional comparison interpolation theorem supplies zh=Ih,0ζe∈Yh and the displayed CDhsℓΩ1−s estimate (Zero-boundary fractional interpolation in the Nitsche comparison norm).

[F8]

For the nonempty domain, C∂≥1; the forms have one volume term, two consistency flux terms, and one penalty term with weights matching ∥⋅∥#,h (Global boundary-flux estimate on a matching mesh, Symmetric and nonsymmetric Nitsche boundary forms).

[A1]

The adjoint solution satisfies ∥ζe∥H1+s(Ω)≤CR∥e∥2 for some fixed CR and s∈(1/2,1]. This dual elliptic regularity is an explicit PDE hypothesis, not a consequence of the variational adjoint equation.

[A3]

The primal solution satisfies the energy theorem's comparison-norm approximation hypothesis, so its conditional conclusion gives ∥e∥#,h≤CθCI(∑K∈ThhK2t∥u∥H1+t(K)2)1/2 (Nitsche consistency and energy quasi-optimality).

Proof

technique · symmetric adjoint consistency and duality

Given: Countable Choice; e, ζe, the hypotheses in the Statement, [F1]–[F8], [A1], and [A3] for the final conditional branch.

1.1F2F6given

The adjoint equation is bounded and coercive on the Hilbert space H01(Ω): Cauchy–Schwarz bounds the gradient form, and [F2] plus Poincaré makes it coercive in the usual H1 norm. Its load v↦∫Ωve is bounded by ∥v∥H1∥e∥2, so [F2] gives a unique weak solution; the stated higher regularity remains an assumption on this solution. Testing the adjoint equation with any ϕ∈Cc∞(Ω)⊂H01(Ω) gives ∫∇ϕ⋅∇ζe=∫ϕe, exactly the distributional identity −Δζe=e. Thus [F6] applies to ζe as well as to u.

1.2F1F5F6givenalgebra

Apply [F6] to ζe with test e. The adjoint equation gives ∥e∥22=∫Ω∇e⋅∇ζe−∑F∫Fe ∂nζe. By [F5], both zh and ζe have zero boundary traces, so ah1(e,zh)=0 from [F1] reduces to ∫Ω∇e⋅∇zh−∑F∫Fe ∂nzh=0; the other terms vanish because their test values are zero. Subtracting this zero identity yields ∥e∥22=ah1(e,ζe−zh).

1.3F3F4F8givenalgebra

By [F3], the regularity of u and ζe places e and ζe−zh in the comparison space Xh of the forms definition; [F4] supplies their facet traces. For arbitrary v,w∈Xh, weighted Cauchy–Schwarz in the form definition bounds the volume product by ∥v∥#,h∥w∥#,h, each of the two flux products by the product of the normal-flux component of one norm and the boundary-value component of the other, and the penalty product by γ0∥v∥#,h∥w∥#,h. Thus ∣ah1(v,w)∣≤(3+γ0)∥v∥#,h∥w∥#,h. By [F8], C∂≥1, so 3+γ0≤2+C∂+γ0=M1. This proves the all-comparison-space bound with the original M1, without applying a discrete inverse estimate to ζe−zh.

2.1A1F7step 1.2step 1.3algebra

Interpolation [F7] and the bound of step 1.3 give ∥e∥22=∣ah1(e,ζe−zh)∣≤M1CDhsℓΩ1−s∥e∥#,h∥ζe∥H1+s. Use [A1]; if ∥e∥2=0 the conclusion is immediate, and otherwise divide by ∥e∥2 to obtain the first estimate.

3.1A3step 2.1algebra∎

Under the separate higher-order primal hypothesis [A3], substitute its energy error bound into the first estimate from step 2.1 and multiply the constants. This gives the stated conditional primal L2 rate without changing its exponent range or local seminorm.

Source notes

Guermond's Chapter 37, Theorem 37.8 cancels the adjoint boundary consistency defect and uses a zero-trace interpolant in a norm controlling both the boundary value and normal-derivative traces. The local fractional weak Green and comparison interpolation suppliers prove those interfaces for the commissioned dual branch. The dual elliptic regularity estimate is still a genuine PDE hypothesis, and the higher-order/local primal branch [A3] is preserved as its own assumption; neither follows from ordinary conforming H1 approximation.

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