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Theorem 1.1 — Possible orders of harmonic maps into Euclidean buildings

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HarmonicBuilding.possibleOrders

by ShouqiaoWang · Aug 26, 2026 · Mathlib c5ea003 (Lean v4.30.0)

calculus-of-variationscoxeter-groupseuclidean-buildingsgeometric-analysisharmonic-maps

Let DDD be a connected domain in a Riemann surface, let XXX be a complete Euclidean building of Coxeter type WWW, and let u:D→Xu:D\to Xu:D→X be a nonconstant energy-minimizing harmonic map in the concrete metric-Sobolev sense fixed by the definition bundle. For every x0∈Dx_0\in Dx0​∈D, prove that the small-scale energy is finite, the relevant boundary moment is positive, and the frequency quotient has a well-defined order. Moreover, prove that there exist positive integers m,km,km,k such that

Ord⁡u(x0)=mkandk∣∣W∣.\operatorname{Ord}_u(x_0)=\frac{m}{k} \qquad\text{and}\qquad k\mid |W|.Ordu​(x0​)=km​andk∣∣W∣.

If XXX has rank one, prove the sharper conclusion

Ord⁡u(x0)=m2for some m≥2.\operatorname{Ord}_u(x_0)=\frac{m}{2} \quad\text{for some }m\ge2.Ordu​(x0​)=2m​for some m≥2.

The nonconstant condition is explicit because the standard frequency quotient for a constant map is 0/00/00/0; it is also the condition used by the source paper's tangent-map reduction.

Preamble
import Definitions.Def_frame_2026_harmonic_building_interfaces
Formal statement
namespace HarmonicBuilding

open scoped Manifold

theorem possibleOrders
    {N : ℕ} (C : EuclideanCoxeterData N)
    {X S : Type*}
    [MetricSpace X] [CompleteSpace X] [MeasurableSpace X] [BorelSpace X]
    [TopologicalSpace S] [T2Space S] [SecondCountableTopology S]
    [ChartedSpace ℂ S] [IsManifold (modelWithCornersSelf ℂ ℂ) ⊤ S]
    (B : EuclideanBuildingData N C X)
    (D : RiemannSurfaceDomain S) (u : S → X) (x₀ : D.Point) :
    PossibleOrdersProblem C B D u x₀ := by sorry

end HarmonicBuilding
Source
Christine Breiner and Ben K. Dees, On the Possible Orders of Harmonic Maps into Euclidean Buildings, Calculus of Variations and Partial Differential Equations (2026), Theorem 1.1 on physical p. 2; definitions and reduction in Section 2: https://doi.org/10.1007/s00526-026-03375-5
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What the Lean code literally says, in plain math · gpt-5.6-sol

For every natural number NNN, every Euclidean Coxeter datum CCC of dimension NNN—in particular N>0N>0N>0, with a concretely represented affine-isometry subgroup generated by a nonempty set of affine reflections, a finite orthogonal subgroup WWW, and a surjective rotational-part homomorphism onto WWW agreeing pointwise with affine linear parts—every complete metric space XXX whose supplied measurable structure is its Borel structure, every Hausdorff second-countable smooth one-dimensional complex manifold SSS, every Euclidean-building datum BBB on XXX whose atlas has pair coverage, ray and line coverage, affine-Weyl-compatible overlaps, maximality among compatible charts, and the stated CAT(0) segment and comparison properties, every connected open domain D⊆SD\subseteq SD⊆S, every map u:S→Xu:S\to Xu:S→X, and every point x0∈Dx_0\in Dx0​∈D, the following implication holds: if uuu is continuous on DDD and, at every point of DDD, its expression in the preferred extended complex chart minimizes the normalized KS liminf energy on some coordinate ball against every KS-Sobolev competitor having vanishing normalized shrinking-annulus trace distance, and if there exist x,y∈Dx,y\in Dx,y∈D with u(x)≠u(y)u(x)\ne u(y)u(x)=u(y), then there is an r0>0r_0>0r0​>0 such that for every 0<r<r00<r<r_00<r<r0​ the closed coordinate ball at x0x_0x0​ lies inside the coordinate image of DDD, the KS energy on its open ball is finite, and the real conversion of the boundary moment is positive; moreover, there exist natural numbers m,km,km,k with m>0m>0m>0, k>0k>0k>0, k≤mk\le mk≤m, and k∣∣W∣k\mid |W|k∣∣W∣ for which the real quotient of rrr times that finite KS energy by the boundary moment tends to m/km/km/k as r→0r\to0r→0 through positive values; and if N=1N=1N=1, there also exists a natural number m′≥2m'\ge2m′≥2 for which the same quotient tends to m′/2m'/2m′/2. Here the coordinate map is the total composition with the extended chart inverse, the KS energy is the positive-scale liminf of the nested normalized difference-quotient integrals, the boundary moment is rrr times the angular integral of squared distance from the center value, and all divisions are total real divisions, although the OrderDefinedAt conclusion ensures finite energy and a positive finite denominator at sufficiently small positive radii. The building datum BBB is required as an argument but disappears from the unfolded conclusion; the conclusion depends on CCC through NNN and ∣W∣|W|∣W∣. If the harmonicity antecedent is false, or it is true but the explicit nonconstancy antecedent is false, the theorem’s asserted implication is true vacuously. The rank-one numerator m′m'm′ is existentially independent of the earlier m,km,km,k.

Human review
  • Endorsed by Shuze Chen · Aug 27, 2026

  • Endorsed by ShouqiaoWang · Aug 27, 2026

    Confirmed by the mission captain (proposal self-audit).

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