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We apply this principle to derive regularity results in regimes lying strictly beyond the reach of existing gauge-theoretic methods. As a foundational example, we provide a new direct proof of local Hölder continuity for almost harmonic maps $-\Delta \boldsymbol{u} = |\nabla \boldsymbol{u}|^2 \boldsymbol{u} + \boldsymbol{f}$ into $\mathbb{S}^n$ with $L^q$-integrable tension fields. We then extend the analysis to systems of the form $-\Delta \boldsymbol{u} = \Omega \cdot \nabla \boldsymbol{u} + \boldsymbol{f}$, replacing geometric antisymmetry assumption on the connection form $\Omega \in L^2$ with the purely analytic condition $\mathrm{div} \Omega \in L^q$ for some $q>1$...
From: Giovanni Di Fratta PhD [view email]
[v1]
Sun, 21 Jun 2026 12:27:20 UTC (79 KB)
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