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✓ 4 results · all verified · 2 also independently AI-judged
Every result on this page is machine-checked by a proof checker and read in full and owner-audited; the judge is an additional, independent cross-model AI review of the proofs. The 2 not AI-judged were verified by owner audit (typically over a confirmed judge false positive), not failures.

First-order least-squares FEM and practical DPG — Examples

1 · Prerequisites

2 · Summary

These examples check the boundary and stability caveats. If the homogeneous Dirichlet condition is dropped, constants give distinct zero-residual states for zero data. If the practical test space has smaller dimension than its trial space, the restricted Riesz map has a kernel and unique solvability cannot be guaranteed.

The finite-dimensional DPG calculation compares ideal and practical trial-to-test vectors for the nonsymmetric matrix A=(1101). It yields coefficients 1/2 and 1 under the same load, so the practical method need not reproduce the ideal test vector.

On the unit square with a two-triangle conforming mesh, u=x(1−x)y(1−y), σ=−∇u, and f=2x(1−x)+2y(1−y) give an exact least-squares residual certificate: the scalar vanishes on the boundary, the first residual is zero by construction, and div⁡σ=f.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

CounterexampleConstruction: Literature-sourcedVerification: AI-adaptedprecheck passjudge pass (gpt-6-luna)Open item page →

Dropping the H1-zero boundary condition makes least squares nonunique

Statement

If zero boundary values are removed from the continuous first-order Poisson least-squares problem with zero load, every constant scalar u with σ=0 has zero residual; hence the unconstrained minimizer is not unique.

Facts & Assumptions

Given: The least-squares residual convention and f=0.

[F1]

The residual is (σ+∇u,divσ−f) and the intended scalar space is H01. (First-order least-squares formulation of the Dirichlet Poisson problem)

Proof

1.1F1constructalgebra

Fix any c∈R and set u(x)=c, σ(x)=0, f=0. Then ∇u=0 and divσ=0, so both residual components in [F1] vanish.

2.1step 1.1givenalgebra∎

Distinct constants give distinct H1 functions, and every one has objective zero, the minimum of a sum of squares. They are all admissible after the stated replacement of H1_0 by H1, so the unconstrained minimizer is not unique.

ExampleConstruction: Literature-sourcedVerification: AI-adaptedprecheck passjudge pass (gpt-6-luna)Open item page →

An exact polynomial Poisson solution has a zero residual certificate

Statement

Assume Countable Choice. On Ω=(0,1)2 with its two-triangle diagonal mesh, let u=x(1−x)y(1−y), σ=−∇u, and f=−Δu. Then u∈H01(Ω), σ∈H(div;Ω), σ+∇u=0, and divσ−f=0, so the continuous least-squares residual is zero.

Facts & Assumptions

Given: The square domain and the polynomial fields in the Statement.

[F1]

The first-order Poisson residual and boundary convention. (First-order least-squares formulation of the Dirichlet Poisson problem)

[A1]

Countable Choice is declared by the zero-boundary polynomial density supplier. (The Axiom of Countable Choice (ACω))

[F2]

A conforming piecewise polynomial with zero boundary traces on a finite matching mesh belongs to H01. (Zero-boundary conforming polynomials lie in W0 1p and satisfy Poincare)

[F3]

H01 is the H1 closure of compactly supported smooth functions. (Zero-boundary Sobolev space as a norm closure)

[F4]

H(div) consists of L2 vector fields with L2 distributional divergence. (The real H(div) space)

Proof

1.1A1F1F2F3F4givenalgebra

The factor x(1−x)y(1−y) vanishes on all four edges. Differentiating gives Δu=−2x(1−x)−2y(1−y), so f=2x(1−x)+2y(1−y) is polynomial and [F2] gives u∈H01. For every v∈Cc∞(Ω), integration by parts gives (∇u,∇v)=(f,v); both sides are continuous in the H1 norm, so [F3] extends the identity to every v∈H01. Thus u is the weak Dirichlet solution. Also σ=−∇u and div⁡σ=f are polynomials in L2, so [F4] gives σ∈H(div⁡;Ω).

2.1F1step 1.1algebra∎

By definition σ+∇u=0 and divσ=−Δu=f, so both components in [F1] vanish pointwise. The objective is nonnegative and therefore this exact zero residual is a global least-squares minimum.

CounterexampleConstruction: Literature-sourcedVerification: AI-adaptedprecheck passOpen item page →

A smaller constant test space gives a nontrivial practical DPG kernel

Statement

On one triangle, take a four-dimensional trial subspace of P1(K)2×P0(K) and the three-dimensional constant test space P0(K)2×P0(K). The practical trial-to-test map has a nontrivial kernel, so the normal equations cannot have a unique trial solution for any load for which a solution exists.

Facts & Assumptions

Given: A nondegenerate triangle, the ultraweak form, and the finite Riesz construction.

[F1]

The cell trial/test form and polynomial setting are specified in the DPG formulation. (Ultraweak Poisson DPG spaces and plan-consistent bilinear form)

[F2]

The practical trial-to-test map is the finite Riesz representative. (Exact local finite Riesz solves for practical DPG tests)

Proof

1.1F1constructalgebra

Choose Wh=span⁡{(e1,0),(e2,0),(x1e1,0),(x2e2,0)} in the vector/scalar volume trial variables; these four fields are linearly independent as L2 pairs. The constant test space has dimension 2+1=3.

2.1F2step 1.1algebra∎

In a fixed basis of the constant test space, the Gram matrix is positive definite, and [F2] returns G−1g(w) in that basis. The right-hand side g(w) is linear in w, so the restricted practical trial-to-test map is linear from the four-dimensional trial subspace into the three-dimensional test space. The images of four independent basis vectors are therefore linearly dependent; the corresponding nonzero coefficient vector is in the kernel. The normal matrix is Br∗Br, so this vector has zero quadratic energy; if a solution exists, adding any multiple produces another trial solution.

ExampleConstruction: Literature-sourcedVerification: AI-adaptedprecheck passOpen item page →

An explicit finite model separates ideal and practical test vectors

Statement

Let U=V=R2 with Euclidean inner product, A=(1101), b(x,y)=(Ax)⋅y, Uh=span⁡(e2), practical test space Vr=span⁡(e1), and load F(y)=e1⋅y. Then Te2=(1,1), Tre2=e1, and ideal and practical trial coefficients are 1/2 and 1.

Facts & Assumptions

Given: The stated finite-dimensional trial/test data.

[F1]

In this finite model, define Tw∈V by (Tw,y)V=b(w,y) for every y∈V; existence and uniqueness follow from finite-dimensional Riesz representation. (Finite-dimensional Riesz representation: every functional is uniquely v↦⟨v,w⟩)

[F2]

Define Trw∈Vr by (Trw,y)V=b(w,y) for every y∈Vr; finite-dimensional Riesz representation again gives existence and uniqueness. (Finite-dimensional Riesz representation: every functional is uniquely v↦⟨v,w⟩)

[F3]

Finite-dimensional Riesz systems have unique representatives. (Finite-dimensional Riesz representation: every functional is uniquely v↦⟨v,w⟩)

Proof

1.1F1F2givenalgebra

Ae2=(1,1), so (Ae2,y)V=b(e2,y) for every y∈V, and [F1] gives Te2=(1,1). For every y=te1∈Vr, (e1,y)V=t=b(e2,y), so [F2] gives Tre2=e1.

2.1F1F2F3step 1.1algebra∎

For ideal coefficient c, the equation is b(ce2,Te2)=F(Te2), hence 2c=1 and c=1/2. For practical tests it is b(ce2,e1)=F(e1), hence c=1. Uniqueness follows from the positive Gram scalars 2 and 1 in [F3].

Remarks

The Euclidean Riesz maps defined here give a finite-dimensional analogue of Ideal Poisson DPG trial-to-test Riesz map and Exact local finite Riesz solves for practical DPG tests.

Sources