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The pasted map's energy is at most the sum over the two pieces

Disproved
HarmonicBuilding.ksEnergy_glue_le_annulus

by Shuze Chen · Aug 31, 2026 · Mathlib 0df444a (Lean v4.33.1)

calculus-of-variationsmetric-geometrysobolev-spaces

Let uuu have finite Korevaar--Schoen energy on BR(z)B_R(z)BR​(z), let vvv have finite energy on Br(z)B_r(z)Br​(z) with 0<r<R0<r<R0<r<R, and suppose uuu and vvv have the same Sobolev trace on the circle ∂Br(z)\partial B_r(z)∂Br​(z). Let www be the cut-and-paste map, equal to vvv inside Br(z)B_r(z)Br​(z) and to uuu outside. Then www has finite energy on BR(z)B_R(z)BR​(z), and

E(w;BR(z)) ≤ E(v;Br(z))+E(u;BR(z)∖Br(z)).E\bigl(w;B_R(z)\bigr)\ \le\ E\bigl(v;B_r(z)\bigr)+E\bigl(u;B_R(z)\setminus B_r(z)\bigr).E(w;BR​(z)) ≤ E(v;Br​(z))+E(u;BR​(z)∖Br​(z)).

Role. This is the substantive half of the gluing lemma: the energy of the pasted map on the whole disc is no more than the sum of its energies on the two pieces. It fails without the trace hypothesis — a genuine jump across the circle contributes infinite energy — so this is exactly where matching traces is used. Combined with superadditivity of the energy, which is elementary, it gives the comparison

E(w;BR)+E(u;Br) ≤ E(u;BR)+E(v;Br)E(w;B_R)+E(u;B_r)\ \le\ E(u;B_R)+E(v;B_r)E(w;BR​)+E(u;Br​) ≤ E(u;BR​)+E(v;Br​)

that lets a map minimizing energy at one radius be shown to minimize at every smaller radius.

Formalization note. The approximate energies are not subadditive over a set and its complement, because the density carried by the interface definition is truncated by the very set being integrated over, and that truncation grows with the set. Subadditivity is therefore a statement about the limit, and its proof goes through the Korevaar--Schoen energy measure together with the trace theory of that paper; the interface's finite-energy hypotheses on uuu and vvv are what make the two sides meaningful.


Retired 2026-09-07 — disproved, false as formalized. Do not use as a dependency.

The Korevaar--Schoen gluing inequality itself is standard and correct; what fails is the binding. The lemma layer binds [MeasurableSpace X] with no compatibility between that sigma-algebra and the metric on X, whereas the mission's goal-level predicate PossibleOrdersProblem carries [BorelSpace X]. IsKSSobolevOn, IsPlanarKSHarmonicAt and IsKSHarmonic do not, so the energy integrals can be made to degenerate on a pathological sigma-algebra.

A faithful restatement needs [BorelSpace X] (and, for the harmonicity predicates, continuity -- see the sibling retirements in this family). No corrected replacement node exists yet.

Preamble
import Definitions.Def_frame_2026_harmonic_building_interfaces
Formal statement
namespace HarmonicBuilding

universe u

theorem ksEnergy_glue_le_annulus {X : Type u} [PseudoMetricSpace X]
    [MeasurableSpace X]
    (Omega : Set ℂ) (u v : ℂ → X) (z : ℂ) (r R : ℝ)
    (hr : 0 < r) (hrR : r < R)
    (hball : Metric.closedBall z R ⊆ Omega)
    (hu : IsKSSobolevOn Omega (Metric.ball z R) u)
    (hv : IsKSSobolevOn Omega (Metric.ball z r) v)
    (htr : SameKSTraceOnCircle u v z r) :
    IsKSSobolevOn Omega (Metric.ball z R)
        (fun w => if dist w z < r then v w else u w) ∧
      ksEnergy Omega (Metric.ball z R)
          (fun w => if dist w z < r then v w else u w)
        ≤ ksEnergy Omega (Metric.ball z r) v
          + ksEnergy Omega (Metric.ball z R \ Metric.ball z r) u := by sorry

end HarmonicBuilding
Source
N. Korevaar and R. Schoen, Sobolev spaces and harmonic maps for metric space targets, Comm. Anal. Geom. 1 (1993), Sections 1.5 and 1.12.

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