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CounterexampleConstruction: Literature-sourcedVerification: AI-adaptedPipeline-generatedverified 2026-10-22 (gpt-6.1-sol)
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A shrinking inclusion rules out uniform Lipschitz stability on the BV class

Statement refuted

Assume the Axiom of Choice and Countable Choice. Let D=B(x0,a)⊂(0,1)2 with x0=(1/2,1/2) and a=1/4, let D′=B(x0,a/2), and set m=1/2, M=3/2, and R=1. There exists a finite constant L such that ∥γ1−γ2∥L2(D)≤L∥Λ˙γ1−Λ˙γ2∥L(D(D)/C1,(D(D)/C1)∗) for every γ1,γ2∈X2(1).

Facts & Assumptions

Given: The Axiom of Choice and Countable Choice; D=B(x0,a), a=1/4, D′=B(x0,a/2), m=1/2, M=3/2, R=1, γ0≡1, and γj=1+12χB(x0,rj) with rj=a/2j+2.

[F1]

The class X2(1) uses the bounds 1/2≤γ≤3/2, background value 1 off D′, and max⁡{∥γ∥L1(D),TV(γ;D)}≤1. (Calderón admissible conductivity classes)

[F2]

For each 0<r≤a/2 and β>0, the disk inclusion 1+βχB(x0,r) has DN eigenvalue difference from the background disk equal to 2naη(r/a)2n1−η(r/a)2n on mode n≥1, and the induced quotient-space operator norm is at most 2η1−η(r/a)2, where η=β/(2+β). (DN spectrum of a concentric radial conductivity inclusion)

[F3]

The weak DN maps are bounded operators on the trace quotient and are uniquely defined for these uniformly elliptic conductivities. (Weak Dirichlet-to-Neumann map for bounded conductivities, Well-posedness of the weak conductivity Dirichlet-to-Neumann map)

[F4]

For every disk B(x0,r), its indicator has total variation 2πr in the plane. (Scaling the perimeter of a disk inclusion)

[A1]

The Axiom of Choice is assumed at the weak DN interface, and Countable Choice at the disk-perimeter scaling and Fourier trace-quotient interfaces. (The Axiom of Choice, The Axiom of Countable Choice (ACω))

Counterexample

technique · direct

Given: The data in the Statement refuted.

1.1A1F1F4givenalgebra

For every j≥1, rj≤a/8<a/2, so the inclusion lies in D′. Its values are 1 and 3/2, and its L1(D) norm is πa2+12πrj2≤π/16+π/2048<1. By [F4], TV(γj;D)=12(2πrj)=πrj≤πa/8<1. Also γ0 equals the background and has L1(D)=π/16<1 and zero variation. Thus [F1] gives γ0,γj∈X2(1).

1.2A1F2F3givenalgebra

The squared L2(D) difference is ∫B(x0,rj)(1/2)2dx=πrj2/4, hence its norm is 12πrj. Apply [F2] with β=1/2, so η=(1/2)/(5/2)=1/5 and 2η/(1−η)=1/2; this gives the stated DN bound. The well-posedness and definition facts [F3] ensure the operator comparison is in the stated quotient-space norm.

2.1F3step 1.1step 1.2algebra∎

If the asserted finite constant K existed, step 1.1 puts both coefficients in its class, while step 1.2 computes the data and DN differences; hence the estimate applied to (γj,γ0) would give 12πrj≤K2(rj/a)2. Dividing by rj>0 yields π≤Krj/a2 for every j. Since rj→0, the right-hand side tends to zero, contradicting π>0. Therefore the refuted statement is false.

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